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rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24776" xmlns="http://purl.org/rss/1.0/"><title>A new susceptibility-weighted image reconstruction method for the reduction of background phase artifacts</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24776</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A new susceptibility-weighted image reconstruction method for the reduction of background phase artifacts</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yoojin Lee, Yeji Han, HyunWook Park</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-14T09:26:01.864606-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24776</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24776</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24776</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24776-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To significantly reduce the background phase effects, especially at the air–tissue interface, and to enhance the desirable local structures of veins in susceptibility-weighted imaging.</p></div></div>
<div class="section" id="mrm24776-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>In the proposed reconstruction method called Magnitude of Complex Filtering, a complex-valued magnetic resonance image is acquired using a flow-compensated high-resolution 3D gradient-echo sequence and the magnitude of the complex-valued image is set to 1 so that the phase information, which contains details of the local susceptibility, is emphasized. Then, the nonlinear filter of the Magnitude of Complex Filtering method is applied to the complex-valued image with a constant magnitude. This filter utilizes the magnitude of the low-pass and high-pass filtered complex data to selectively reduce the background phase effects while enhancing the local structures. The filter output is then processed to generate a susceptibility-weighted image.</p></div></div>
<div class="section" id="mrm24776-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Compared with the conventional susceptibility-weighted images generated by a homodyne high-pass filter, the susceptibility-weighted images from the proposed Magnitude of Complex Filtering method show significant improvement; the undesirable artifacts at the air–tissue interface regions and the brain boundaries are significantly reduced, while the contrast of the local structures of veins is enhanced.</p></div></div>
<div class="section" id="mrm24776-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The Magnitude of Complex Filtering method successfully reduced most background phase effects without requiring additional processing or scan time. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
To significantly reduce the background phase effects, especially at the air–tissue interface, and to enhance the desirable local structures of veins in susceptibility-weighted imaging.


Methods
In the proposed reconstruction method called Magnitude of Complex Filtering, a complex-valued magnetic resonance image is acquired using a flow-compensated high-resolution 3D gradient-echo sequence and the magnitude of the complex-valued image is set to 1 so that the phase information, which contains details of the local susceptibility, is emphasized. Then, the nonlinear filter of the Magnitude of Complex Filtering method is applied to the complex-valued image with a constant magnitude. This filter utilizes the magnitude of the low-pass and high-pass filtered complex data to selectively reduce the background phase effects while enhancing the local structures. The filter output is then processed to generate a susceptibility-weighted image.


Results
Compared with the conventional susceptibility-weighted images generated by a homodyne high-pass filter, the susceptibility-weighted images from the proposed Magnitude of Complex Filtering method show significant improvement; the undesirable artifacts at the air–tissue interface regions and the brain boundaries are significantly reduced, while the contrast of the local structures of veins is enhanced.


Conclusion
The Magnitude of Complex Filtering method successfully reduced most background phase effects without requiring additional processing or scan time. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24745" xmlns="http://purl.org/rss/1.0/"><title>Efficient concomitant and remanence field artifact reduction in ultra-low-field MRI using a frequency-space formulation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24745</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Efficient concomitant and remanence field artifact reduction in ultra-low-field MRI using a frequency-space formulation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yi-Cheng Hsu, Panu T. Vesanen, Jaakko O. Nieminen, Koos C.J. Zevenhoven, Juhani Dabek, Lauri Parkkonen, I-Liang Chern, Risto J. Ilmoniemi, Fa-Hsuan Lin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-13T16:39:40.951949-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24745</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24745</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24745</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24745-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>For ultra-low-field MRI, the spatial-encoding magnetic fields generated by gradient coils can have strong concomitant fields leading to prominent image distortion. Additionally, using superconducting magnet to pre-polarize magnetization can improve the signal-to-noise ratio of ultra-low-field MRI. Yet the spatially inhomogeneous remanence field due to the permanently trapped flux inside a superconducting pre-polarizing coil modulates magnetization and causes further image distortion.</p></div></div>
<div class="section" id="mrm24745-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Method</h4><div class="para"><p>We propose a two-stage frequency–space (<em>f–x</em>) formulation to accurately describe the dynamics of spatially-encoded magnetization under the influence of concomitant and remanence fields, which allows for correcting image distortion due to concomitant and remanence fields.</p></div></div>
<div class="section" id="mrm24745-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Our method is computationally efficient as it uses a combination of the fast Fourier transform algorithm and a linear equation solver. With sufficiently dense discretization in solving the linear equation, the performance of this <em>f–x</em> method was found to be stable among different choices of the regularization parameter and the regularization matrix.</p></div></div>
<div class="section" id="mrm24745-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>We present this method together with numerical simulations and experimental data to demonstrate how concomitant and remanence field artifacts in ultra-low-field MRI can be corrected efficiently. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
For ultra-low-field MRI, the spatial-encoding magnetic fields generated by gradient coils can have strong concomitant fields leading to prominent image distortion. Additionally, using superconducting magnet to pre-polarize magnetization can improve the signal-to-noise ratio of ultra-low-field MRI. Yet the spatially inhomogeneous remanence field due to the permanently trapped flux inside a superconducting pre-polarizing coil modulates magnetization and causes further image distortion.


Method
We propose a two-stage frequency–space (f–x) formulation to accurately describe the dynamics of spatially-encoded magnetization under the influence of concomitant and remanence fields, which allows for correcting image distortion due to concomitant and remanence fields.


Results
Our method is computationally efficient as it uses a combination of the fast Fourier transform algorithm and a linear equation solver. With sufficiently dense discretization in solving the linear equation, the performance of this f–x method was found to be stable among different choices of the regularization parameter and the regularization matrix.


Conclusion
We present this method together with numerical simulations and experimental data to demonstrate how concomitant and remanence field artifacts in ultra-low-field MRI can be corrected efficiently. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24773" xmlns="http://purl.org/rss/1.0/"><title>Analysis and correction of gradient nonlinearity bias in apparent diffusion coefficient measurements</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24773</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Analysis and correction of gradient nonlinearity bias in apparent diffusion coefficient measurements</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dariya I. Malyarenko, Brian D. Ross, Thomas L. Chenevert</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-13T16:39:35.774975-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24773</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24773</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24773</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">0n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">0n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24773-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Gradient nonlinearity of MRI systems leads to spatially dependent <em>b</em>-values and consequently high non-uniformity errors (10–20%) in apparent diffusion coefficient (ADC) measurements over clinically relevant field-of-views. This work seeks practical correction procedure that effectively reduces observed ADC bias for media of arbitrary anisotropy in the fewest measurements.</p></div></div>
<div class="section" id="mrm24773-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>All-inclusive bias analysis considers spatial and time-domain cross-terms for diffusion and imaging gradients. The proposed correction is based on rotation of the gradient nonlinearity tensor into the diffusion gradient frame where spatial bias of <b><em>b</em></b>-matrix can be approximated by its Euclidean norm. Correction efficiency of the proposed procedure is numerically evaluated for a range of model diffusion tensor anisotropies and orientations.</p></div></div>
<div class="section" id="mrm24773-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Spatial dependence of nonlinearity correction terms accounts for the bulk (75–95%) of ADC bias for FA = 0.3–0.9. Residual ADC non-uniformity errors are amplified for anisotropic diffusion. This approximation obviates need for full diffusion tensor measurement and diagonalization to derive a corrected ADC. Practical scenarios are outlined for implementation of the correction on clinical MRI systems.</p></div></div>
<div class="section" id="mrm24773-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>The proposed simplified correction algorithm appears sufficient to control ADC non-uniformity errors in clinical studies using three orthogonal diffusion measurements. The most efficient reduction of ADC bias for anisotropic medium is achieved with non-lab-based diffusion gradients. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Gradient nonlinearity of MRI systems leads to spatially dependent b-values and consequently high non-uniformity errors (10–20%) in apparent diffusion coefficient (ADC) measurements over clinically relevant field-of-views. This work seeks practical correction procedure that effectively reduces observed ADC bias for media of arbitrary anisotropy in the fewest measurements.


Methods
All-inclusive bias analysis considers spatial and time-domain cross-terms for diffusion and imaging gradients. The proposed correction is based on rotation of the gradient nonlinearity tensor into the diffusion gradient frame where spatial bias of b-matrix can be approximated by its Euclidean norm. Correction efficiency of the proposed procedure is numerically evaluated for a range of model diffusion tensor anisotropies and orientations.


Results
Spatial dependence of nonlinearity correction terms accounts for the bulk (75–95%) of ADC bias for FA = 0.3–0.9. Residual ADC non-uniformity errors are amplified for anisotropic diffusion. This approximation obviates need for full diffusion tensor measurement and diagonalization to derive a corrected ADC. Practical scenarios are outlined for implementation of the correction on clinical MRI systems.


Conclusions
The proposed simplified correction algorithm appears sufficient to control ADC non-uniformity errors in clinical studies using three orthogonal diffusion measurements. The most efficient reduction of ADC bias for anisotropic medium is achieved with non-lab-based diffusion gradients. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24783" xmlns="http://purl.org/rss/1.0/"><title>Toward real-time availability of 3D temperature maps created with temporally constrained reconstruction</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24783</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Toward real-time availability of 3D temperature maps created with temporally constrained reconstruction</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nick Todd, Jaya Prakash, Henrik Odéen, Josh Bever, Allison Payne, Phaneendra Yalavarthy, Dennis L. Parker</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-13T16:38:53.7554-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24783</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24783</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24783</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24783-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To extend the previously developed temporally constrained reconstruction (TCR) algorithm to allow for real-time availability of three-dimensional (3D) temperature maps capable of monitoring MR-guided high intensity focused ultrasound applications.</p></div></div>
<div class="section" id="mrm24783-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A real-time TCR (RT-TCR) algorithm is developed that only uses current and previously acquired undersampled k-space data from a 3D segmented EPI pulse sequence, with the image reconstruction done in a graphics processing unit implementation to overcome computation burden. Simulated and experimental data sets of HIFU heating are used to evaluate the performance of the RT-TCR algorithm.</p></div></div>
<div class="section" id="mrm24783-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The simulation studies demonstrate that the RT-TCR algorithm has subsecond reconstruction time and can accurately measure HIFU-induced temperature rises of 20°C in 15 s for 3D volumes of 16 slices (RMSE = 0.1°C), 24 slices (RMSE = 0.2°C), and 32 slices (RMSE = 0.3°C). Experimental results in ex vivo porcine muscle demonstrate that the RT-TCR approach can reconstruct temperature maps with 192 × 162 × 66 mm 3D volume coverage, 1.5 × 1.5 × 3.0 mm resolution, and 1.2-s scan time with an accuracy of ±0.5°C.</p></div></div>
<div class="section" id="mrm24783-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The RT-TCR algorithm offers an approach to obtaining large coverage 3D temperature maps in real-time for monitoring MR-guided high intensity focused ultrasound treatments. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To extend the previously developed temporally constrained reconstruction (TCR) algorithm to allow for real-time availability of three-dimensional (3D) temperature maps capable of monitoring MR-guided high intensity focused ultrasound applications.


Methods
A real-time TCR (RT-TCR) algorithm is developed that only uses current and previously acquired undersampled k-space data from a 3D segmented EPI pulse sequence, with the image reconstruction done in a graphics processing unit implementation to overcome computation burden. Simulated and experimental data sets of HIFU heating are used to evaluate the performance of the RT-TCR algorithm.


Results
The simulation studies demonstrate that the RT-TCR algorithm has subsecond reconstruction time and can accurately measure HIFU-induced temperature rises of 20°C in 15 s for 3D volumes of 16 slices (RMSE = 0.1°C), 24 slices (RMSE = 0.2°C), and 32 slices (RMSE = 0.3°C). Experimental results in ex vivo porcine muscle demonstrate that the RT-TCR approach can reconstruct temperature maps with 192 × 162 × 66 mm 3D volume coverage, 1.5 × 1.5 × 3.0 mm resolution, and 1.2-s scan time with an accuracy of ±0.5°C.


Conclusion
The RT-TCR algorithm offers an approach to obtaining large coverage 3D temperature maps in real-time for monitoring MR-guided high intensity focused ultrasound treatments. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24785" xmlns="http://purl.org/rss/1.0/"><title>Mapping mean and fluctuating velocities by Bayesian multipoint MR velocity encoding-validation against 3D particle tracking velocimetry</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24785</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Mapping mean and fluctuating velocities by Bayesian multipoint MR velocity encoding-validation against 3D particle tracking velocimetry</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Verena Knobloch, Christian Binter, Utku Gülan, Andreas Sigfridsson, Markus Holzner, Beat Lüthi, Sebastian Kozerke</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-13T16:38:45.027925-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24785</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24785</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24785</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24785-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To validate Bayesian multipoint MR velocity encoding against particle tracking velocimetry for measuring velocity vector fields and fluctuating velocities in a realistic aortic model.</p></div></div>
<div class="section" id="mrm24785-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>An elastic cast of a human aortic arch equipped with an 80 or 64% stenotic section was driven by a pulsatile pump. Peak velocities and peak turbulent kinetic energies of more than 3 m/s and 1000 J/m<sup>3</sup> could be generated. Velocity vector fields and fluctuating velocities were assessed using Bayesian multipoint MR velocity encoding with varying numbers of velocity encoding points and particle tracking velocimetry in the ascending aorta.</p></div></div>
<div class="section" id="mrm24785-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Velocities and turbulent kinetic energies measured with 5-fold k-t undersampled 10-point MR velocity encoding and particle tracking velocimetry were found to reveal good correlation with mean differences of −4.8 ± 13.3 cm/s and <em>r</em><sup>2</sup> = 0.98 for velocities and −21.8 ± 53.9 J/m<sup>3</sup> and <em>r</em><sup>2</sup> = 0.98 for turbulent kinetic energies, respectively. Three-dimensional velocity patterns of fast flow downstream of the stenoses and regions of elevated velocity fluctuations were found to agree well.</p></div></div>
<div class="section" id="mrm24785-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Accelerated Bayesian multipoint MR velocity encoding has been demonstrated to be accurate for assessing mean and fluctuating velocities against the reference standard particle tracking velocimetry. The MR method holds considerable potential to map velocity vector fields and turbulent kinetic energies in clinically feasible exam times of &lt;15 min. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To validate Bayesian multipoint MR velocity encoding against particle tracking velocimetry for measuring velocity vector fields and fluctuating velocities in a realistic aortic model.


Methods
An elastic cast of a human aortic arch equipped with an 80 or 64% stenotic section was driven by a pulsatile pump. Peak velocities and peak turbulent kinetic energies of more than 3 m/s and 1000 J/m3 could be generated. Velocity vector fields and fluctuating velocities were assessed using Bayesian multipoint MR velocity encoding with varying numbers of velocity encoding points and particle tracking velocimetry in the ascending aorta.


Results
Velocities and turbulent kinetic energies measured with 5-fold k-t undersampled 10-point MR velocity encoding and particle tracking velocimetry were found to reveal good correlation with mean differences of −4.8 ± 13.3 cm/s and r2 = 0.98 for velocities and −21.8 ± 53.9 J/m3 and r2 = 0.98 for turbulent kinetic energies, respectively. Three-dimensional velocity patterns of fast flow downstream of the stenoses and regions of elevated velocity fluctuations were found to agree well.


Conclusion
Accelerated Bayesian multipoint MR velocity encoding has been demonstrated to be accurate for assessing mean and fluctuating velocities against the reference standard particle tracking velocimetry. The MR method holds considerable potential to map velocity vector fields and turbulent kinetic energies in clinically feasible exam times of &lt;15 min. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24765" xmlns="http://purl.org/rss/1.0/"><title>Background field removal using spherical mean value filtering and Tikhonov regularization</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24765</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Background field removal using spherical mean value filtering and Tikhonov regularization</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hongfu Sun, Alan H. Wilman</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-10T14:03:02.844868-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24765</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24765</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24765</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24765-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To introduce a new method for removing background artifacts in field maps and apply it to enhance the accuracy of susceptibility mapping.</p></div></div>
<div class="section" id="mrm24765-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A field artifact removal method is introduced that is based on the sophisticated harmonic artifact reduction for phase data (SHARP) method exploiting the harmonic mean value property. The new method uses Tikhonov regularization at the deconvolution stage and is referred to as regularization enabled SHARP (RESHARP). RESHARP was compared with SHARP in a field-forward susceptibility simulation and in human brain experiments, considering effects on both field maps and the resulting susceptibility maps.</p></div></div>
<div class="section" id="mrm24765-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>From the simulation, RESHARP was able to reduce error in the field map by 17.4% as compared with SHARP, resulting in a more accurate single-angle susceptibility map with 6.5% relative error (compared with 48.5% using SHARP). Using RESHARP in vivo, field and susceptibility maps of the brain displayed fewer artifacts particularly at the brain boundaries, and susceptibility measurements of iron-rich deep gray matter were also more consistent than SHARP across healthy subjects of similar age.</p></div></div>
<div class="section" id="mrm24765-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Compared with SHARP, RESHARP removes background field artifact more effectively, leading to more accurate susceptibility measurements in iron-rich deep gray matter. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To introduce a new method for removing background artifacts in field maps and apply it to enhance the accuracy of susceptibility mapping.


Methods
A field artifact removal method is introduced that is based on the sophisticated harmonic artifact reduction for phase data (SHARP) method exploiting the harmonic mean value property. The new method uses Tikhonov regularization at the deconvolution stage and is referred to as regularization enabled SHARP (RESHARP). RESHARP was compared with SHARP in a field-forward susceptibility simulation and in human brain experiments, considering effects on both field maps and the resulting susceptibility maps.


Results
From the simulation, RESHARP was able to reduce error in the field map by 17.4% as compared with SHARP, resulting in a more accurate single-angle susceptibility map with 6.5% relative error (compared with 48.5% using SHARP). Using RESHARP in vivo, field and susceptibility maps of the brain displayed fewer artifacts particularly at the brain boundaries, and susceptibility measurements of iron-rich deep gray matter were also more consistent than SHARP across healthy subjects of similar age.


Conclusion
Compared with SHARP, RESHARP removes background field artifact more effectively, leading to more accurate susceptibility measurements in iron-rich deep gray matter. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24755" xmlns="http://purl.org/rss/1.0/"><title>Indexed distribution analysis significance improved significance testing of heterogeneous parameter maps for testing of spatially heterogeneous parameter maps: Application to dynamic contrast-enhanced MRI biomarkers</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24755</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Indexed distribution analysis significance improved significance testing of heterogeneous parameter maps for testing of spatially heterogeneous parameter maps: Application to dynamic contrast-enhanced MRI biomarkers</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Chris J. Rose, James P. B. O'Connor, Tim F. Cootes, Chris J. Taylor, Gordon C. Jayson, Geoff J. M. Parker, John C. Waterton</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-10T12:15:53.129797-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24755</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24755</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24755</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24755-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To develop significance testing methodology applicable to spatially heterogeneous parametric maps of biophysical and physiological measurements arising from imaging studies.</p></div></div>
<div class="section" id="mrm24755-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory</h4><div class="para"><p>Heterogeneity can confound statistical analyses. Indexed distribution analysis (IDA) transforms a reference distribution, establishing correspondences across parameter maps to which significance tests are applied.</p></div></div>
<div class="section" id="mrm24755-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Well-controlled simulated and clinical <em>K</em><sup>trans</sup> data from a dynamic contrast-enhanced magnetic resonance imaging study of bevacizumab were analyzed using conventional significance tests of parameter averages, histogram analysis, and IDA. Repeated pretreatment scans provided negative control; a post treatment scan provided positive control.</p></div></div>
<div class="section" id="mrm24755-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Histogram analysis was insensitive to simulated and known effects. Simulation: conventional analysis identified treatment effect (<em>P</em> ≈ 5 × 10<sup>−4</sup>) and direction, but underestimated magnitude (relative error 67–81%); IDA identified treatment effect (<em>P</em> = 0.001), magnitude, direction, and spatial extent (100% accuracy). Bevacizumab: conventional analysis was sensitive to treatment effect (<em>P</em> = 0.01; 95% confidence interval on <em>K</em><sup>trans</sup> decrease: 23–37%); IDA was sensitive to treatment effect (<em>P</em> &lt; 0.05; <em>K</em><sup>trans</sup> decrease approximately 25%), inferred its spatial extent to be 94–96%, and inferred that <em>K</em><sup>trans</sup> decrease is independent of baseline value, an inference that conventional and histogram analyses cannot make.</p></div></div>
<div class="section" id="mrm24755-sec-0005" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>In the presence of heterogeneity, IDA can accurately infer the magnitude, direction, and spatial extent of between samples of parametric maps, which can be visualized spatially with respect to the original parameter maps. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To develop significance testing methodology applicable to spatially heterogeneous parametric maps of biophysical and physiological measurements arising from imaging studies.


Theory
Heterogeneity can confound statistical analyses. Indexed distribution analysis (IDA) transforms a reference distribution, establishing correspondences across parameter maps to which significance tests are applied.


Methods
Well-controlled simulated and clinical Ktrans data from a dynamic contrast-enhanced magnetic resonance imaging study of bevacizumab were analyzed using conventional significance tests of parameter averages, histogram analysis, and IDA. Repeated pretreatment scans provided negative control; a post treatment scan provided positive control.


Results
Histogram analysis was insensitive to simulated and known effects. Simulation: conventional analysis identified treatment effect (P ≈ 5 × 10−4) and direction, but underestimated magnitude (relative error 67–81%); IDA identified treatment effect (P = 0.001), magnitude, direction, and spatial extent (100% accuracy). Bevacizumab: conventional analysis was sensitive to treatment effect (P = 0.01; 95% confidence interval on Ktrans decrease: 23–37%); IDA was sensitive to treatment effect (P &lt; 0.05; Ktrans decrease approximately 25%), inferred its spatial extent to be 94–96%, and inferred that Ktrans decrease is independent of baseline value, an inference that conventional and histogram analyses cannot make.


Conclusions
In the presence of heterogeneity, IDA can accurately infer the magnitude, direction, and spatial extent of between samples of parametric maps, which can be visualized spatially with respect to the original parameter maps. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24748" xmlns="http://purl.org/rss/1.0/"><title>Rapid estimation of cartilage T2 with reduced T1 sensitivity using double echo steady state imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24748</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Rapid estimation of cartilage T2 with reduced T1 sensitivity using double echo steady state imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rahel Heule, Carl Ganter, Oliver Bieri</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-10T12:15:42.79965-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24748</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24748</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24748</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24748-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>In principle, double echo steady state (DESS) offers morphological and quantitative <em>T</em><sub>2</sub> imaging of cartilage within one single scan. However, accurate <em>T</em><sub>2</sub> estimation is hampered by its prominent <em>T</em><sub>1</sub> dependency in the limit of low flip angles, generally used to image cartilage morphology, as for the osteoarthritis initiative. A new postprocessing approach is introduced to overcome this <em>T</em><sub>1</sub>-related bias for rapid DESS-based <em>T</em><sub>2</sub> quantification in the low flip angle regime.</p></div></div>
<div class="section" id="mrm24748-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Based on a rough global <em>T</em><sub>1</sub> estimator and a golden section search, <em>T</em><sub>2</sub> is extracted from the ratio of the two echoes acquired with DESS. The new relaxometry method is evaluated from simulations and in vivo 3D measurements of the knee joint at 3T.</p></div></div>
<div class="section" id="mrm24748-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>A pronounced reduction in the <em>T</em><sub>1</sub>-related bias of DESS-<em>T</em><sub>2</sub> estimation and increased zonal variation in <em>T</em><sub>2</sub> between deep and superficial cartilage layers are observed. The improvement becomes particularly evident in the range of low flip angles (<em>α</em> &lt; 45°), commonly used for morphological DESS imaging.</p></div></div>
<div class="section" id="mrm24748-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Using a simple global <em>T</em><sub>1</sub> estimate, the reliability of DESS-<em>T</em><sub>2</sub> quantification can be considerably increased. The results emphasize the potential of DESS to fuse accurate quantitative <em>T</em><sub>2</sub> and morphological imaging of the musculoskeletal system within one single scan. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
In principle, double echo steady state (DESS) offers morphological and quantitative T2 imaging of cartilage within one single scan. However, accurate T2 estimation is hampered by its prominent T1 dependency in the limit of low flip angles, generally used to image cartilage morphology, as for the osteoarthritis initiative. A new postprocessing approach is introduced to overcome this T1-related bias for rapid DESS-based T2 quantification in the low flip angle regime.


Methods
Based on a rough global T1 estimator and a golden section search, T2 is extracted from the ratio of the two echoes acquired with DESS. The new relaxometry method is evaluated from simulations and in vivo 3D measurements of the knee joint at 3T.


Results
A pronounced reduction in the T1-related bias of DESS-T2 estimation and increased zonal variation in T2 between deep and superficial cartilage layers are observed. The improvement becomes particularly evident in the range of low flip angles (α &lt; 45°), commonly used for morphological DESS imaging.


Conclusion
Using a simple global T1 estimate, the reliability of DESS-T2 quantification can be considerably increased. The results emphasize the potential of DESS to fuse accurate quantitative T2 and morphological imaging of the musculoskeletal system within one single scan. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24770" xmlns="http://purl.org/rss/1.0/"><title>Chemical exchange saturation transfer effect in blood</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24770</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Chemical exchange saturation transfer effect in blood</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Shaokuan Zheng, Imramsjah M. J. van der Bom, Zhongliang Zu, Guoxing Lin, Yansong Zhao, Matthew J. Gounis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-09T12:26:31.995958-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24770</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24770</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24770</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24770-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>In this report, the feasibility of using blood as an agent for Chemical Exchange Saturation Transfer (CEST) effect is investigated.</p></div></div>
<div class="section" id="mrm24770-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The CEST effect of porcine blood samples was investigated on a 3.0 T MRI scanner using various power levels and on a 14.1 T NMR spectrometer. As a proof-of-concept that CEST can be used to image blood in vivo, the technique was applied in two locations of healthy human volunteers, namely, the femoral artery and the M1-segment of the middle cerebral artery.</p></div></div>
<div class="section" id="mrm24770-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The blood sample experiments showed that maximum CEST Magnetization Transfer Ratio asymmetry (MTR<sub>asym</sub>) values of ∼ 12% were achieved, with likely contributions from multiple blood components. These findings were confirmed during the in vivo experiments where CEST signal of blood was clearly greater than surrounding muscular (2%) and brain tissue (3%).</p></div></div>
<div class="section" id="mrm24770-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Ex vivo and in vivo results show that blood is a suitable CEST agent that generates sufficient CEST contrast relative to surrounding tissue.</p></div></div>
]]></content:encoded><description>

Purpose
In this report, the feasibility of using blood as an agent for Chemical Exchange Saturation Transfer (CEST) effect is investigated.


Methods
The CEST effect of porcine blood samples was investigated on a 3.0 T MRI scanner using various power levels and on a 14.1 T NMR spectrometer. As a proof-of-concept that CEST can be used to image blood in vivo, the technique was applied in two locations of healthy human volunteers, namely, the femoral artery and the M1-segment of the middle cerebral artery.


Results
The blood sample experiments showed that maximum CEST Magnetization Transfer Ratio asymmetry (MTRasym) values of ∼ 12% were achieved, with likely contributions from multiple blood components. These findings were confirmed during the in vivo experiments where CEST signal of blood was clearly greater than surrounding muscular (2%) and brain tissue (3%).


Conclusion
Ex vivo and in vivo results show that blood is a suitable CEST agent that generates sufficient CEST contrast relative to surrounding tissue.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24779" xmlns="http://purl.org/rss/1.0/"><title>3He pO2 mapping is limited by delayed-ventilation and diffusion in chronic obstructive pulmonary disease</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24779</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">3He pO2 mapping is limited by delayed-ventilation and diffusion in chronic obstructive pulmonary disease</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Helen Marshall, Juan Parra-Robles, Martin H. Deppe, David A. Lipson, Rod Lawson, Jim M. Wild</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-09T10:41:52.203435-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24779</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24779</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24779</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24779-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Lung pO<sub>2</sub> mapping with <sup>3</sup>He MRI assumes that the sources of signal decay with time during a breath-hold are radiofrequency depolarization and oxygen-dependent <em>T</em><sub>1</sub> relaxation, but the method is sensitive to other sources of spatio-temporal signal change such as diffusion. The purpose of this work was to assess the use of <sup>3</sup>He pO<sub>2</sub> mapping in patients with chronic obstructive pulmonary disease.</p></div></div>
<div class="section" id="mrm24779-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Ten patients with moderate to severe chronic obstructive pulmonary disease were scanned with a 3D single breath-hold pO<sub>2</sub> mapping sequence.</p></div></div>
<div class="section" id="mrm24779-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Images showed signal increasing over time in some lung regions due to delayed ventilation during breath-hold. Regions of physically unrealistic negative pO<sub>2</sub> values were seen in all patients, and regional mean pO<sub>2</sub> values of −0.3 bar were measured in the two patients most affected by delayed ventilation (where mean time to signal onset was 3–4 s).</p></div></div>
<div class="section" id="mrm24779-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>Movement of gas within the lungs during breath-hold causes regional changes in signal over time that are not related to oxygen concentration, leading to erroneous pO<sub>2</sub> measurements using the linear oxygen-dependent signal decay model. These spatio-temporal sources of signal change cannot be reliably separated at present, making pO<sub>2</sub> mapping using this methodology unreliable in chronic obstructive pulmonary disease patients with significant bullous emphysema or delayed ventilation. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Lung pO2 mapping with 3He MRI assumes that the sources of signal decay with time during a breath-hold are radiofrequency depolarization and oxygen-dependent T1 relaxation, but the method is sensitive to other sources of spatio-temporal signal change such as diffusion. The purpose of this work was to assess the use of 3He pO2 mapping in patients with chronic obstructive pulmonary disease.


Methods
Ten patients with moderate to severe chronic obstructive pulmonary disease were scanned with a 3D single breath-hold pO2 mapping sequence.


Results
Images showed signal increasing over time in some lung regions due to delayed ventilation during breath-hold. Regions of physically unrealistic negative pO2 values were seen in all patients, and regional mean pO2 values of −0.3 bar were measured in the two patients most affected by delayed ventilation (where mean time to signal onset was 3–4 s).


Conclusions
Movement of gas within the lungs during breath-hold causes regional changes in signal over time that are not related to oxygen concentration, leading to erroneous pO2 measurements using the linear oxygen-dependent signal decay model. These spatio-temporal sources of signal change cannot be reliably separated at present, making pO2 mapping using this methodology unreliable in chronic obstructive pulmonary disease patients with significant bullous emphysema or delayed ventilation. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24790" xmlns="http://purl.org/rss/1.0/"><title>Cellular imaging and texture analysis distinguish differences in cellular dynamics in mouse brain tumors</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24790</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cellular imaging and texture analysis distinguish differences in cellular dynamics in mouse brain tumors</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lisa M. Gazdzinski, Brian J. Nieman</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-09T10:03:42.236143-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24790</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24790</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24790</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24790-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The heterogeneous tumor cell population and dynamic microenvironment within a tumor lead to regional variations in cell proliferation, migration, and differentiation. In this work, MRI and optical projection tomography were used to examine and compare the redistribution of a cellular label in two mouse glioma models.</p></div></div>
<div class="section" id="mrm24790-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>GL261 and 4C8 glioma cells labeled with iron oxide particles or with a fluorescent probe were injected into the brains of syngeneic mice and allowed to develop into ∼10-mm<sup>3</sup> tumors. Texture analysis was used to quantitatively describe and compare the label distribution patterns in the two tumor types.</p></div></div>
<div class="section" id="mrm24790-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The label was seen to remain predominantly in the tumor core in GL261 tumors, but become more randomly distributed throughout the tumor volume in 4C8 tumors. Histologically, GL261 tumors displayed a more invasive, aggressive phenotype, although the distribution of mitotic cells in the two tumors was similar.</p></div></div>
<div class="section" id="mrm24790-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The redistribution of a cellular label during tumor growth is characteristic of a tumor model. The label distribution map reflects more than simple differences in cell proliferation and is likely influenced by differences in the tumor microenvironment. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The heterogeneous tumor cell population and dynamic microenvironment within a tumor lead to regional variations in cell proliferation, migration, and differentiation. In this work, MRI and optical projection tomography were used to examine and compare the redistribution of a cellular label in two mouse glioma models.


Methods
GL261 and 4C8 glioma cells labeled with iron oxide particles or with a fluorescent probe were injected into the brains of syngeneic mice and allowed to develop into ∼10-mm3 tumors. Texture analysis was used to quantitatively describe and compare the label distribution patterns in the two tumor types.


Results
The label was seen to remain predominantly in the tumor core in GL261 tumors, but become more randomly distributed throughout the tumor volume in 4C8 tumors. Histologically, GL261 tumors displayed a more invasive, aggressive phenotype, although the distribution of mitotic cells in the two tumors was similar.


Conclusion
The redistribution of a cellular label during tumor growth is characteristic of a tumor model. The label distribution map reflects more than simple differences in cell proliferation and is likely influenced by differences in the tumor microenvironment. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24784" xmlns="http://purl.org/rss/1.0/"><title>APT-weighted and NOE-weighted image contrasts in glioma with different RF saturation powers based on magnetization transfer ratio asymmetry analyses</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24784</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">APT-weighted and NOE-weighted image contrasts in glioma with different RF saturation powers based on magnetization transfer ratio asymmetry analyses</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jinyuan Zhou, Xiaohua Hong, Xuna Zhao, Jia-Hong Gao, Jing Yuan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-09T09:50:53.802269-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24784</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24784</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24784</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Rapid Communication</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24784-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To investigate the saturation-power dependence of amide proton transfer (APT)-weighted and nuclear Overhauser enhancement-weighted image contrasts in a rat glioma model at 4.7 T.</p></div></div>
<div class="section" id="mrm24784-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The 9L tumor-bearing rats (<em>n</em> = 8) and fresh chicken eggs (<em>n</em> = 4) were scanned on a 4.7-T animal magnetic resonance imaging scanner. Z-spectra over an offset range of ±6 ppm were acquired with different saturation powers, followed by the magnetization transfer-ratio asymmetry analyses around the water resonance.</p></div></div>
<div class="section" id="mrm24784-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The nuclear Overhauser enhancement signal upfield from the water resonance (−2.5 to −5 ppm) was clearly visible at lower saturation powers (e.g., 0.6 µT) and was larger in the contralateral normal brain tissue than in the tumor. Conversely, the APT effect downfield from the water resonance was maximized at relatively higher saturation powers (e.g., 2.1 µT) and was larger in the tumor than in the contralateral normal brain tissue. The nuclear Overhauser enhancement decreased the APT-weighted image signal, based on the magnetization transfer-ratio asymmetry analysis, but increased the APT-weighted image contrast between the tumor and contralateral normal brain tissue.</p></div></div>
<div class="section" id="mrm24784-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The APT and nuclear Overhauser enhancement image signals in tumor are maximized at different saturation powers. The saturation power of roughly 2 μT is ideal for APT-weighted imaging at clinical <em>B</em><sub>0</sub> field strengths. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To investigate the saturation-power dependence of amide proton transfer (APT)-weighted and nuclear Overhauser enhancement-weighted image contrasts in a rat glioma model at 4.7 T.


Methods
The 9L tumor-bearing rats (n = 8) and fresh chicken eggs (n = 4) were scanned on a 4.7-T animal magnetic resonance imaging scanner. Z-spectra over an offset range of ±6 ppm were acquired with different saturation powers, followed by the magnetization transfer-ratio asymmetry analyses around the water resonance.


Results
The nuclear Overhauser enhancement signal upfield from the water resonance (−2.5 to −5 ppm) was clearly visible at lower saturation powers (e.g., 0.6 µT) and was larger in the contralateral normal brain tissue than in the tumor. Conversely, the APT effect downfield from the water resonance was maximized at relatively higher saturation powers (e.g., 2.1 µT) and was larger in the tumor than in the contralateral normal brain tissue. The nuclear Overhauser enhancement decreased the APT-weighted image signal, based on the magnetization transfer-ratio asymmetry analysis, but increased the APT-weighted image contrast between the tumor and contralateral normal brain tissue.


Conclusion
The APT and nuclear Overhauser enhancement image signals in tumor are maximized at different saturation powers. The saturation power of roughly 2 μT is ideal for APT-weighted imaging at clinical B0 field strengths. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24788" xmlns="http://purl.org/rss/1.0/"><title>Accumulation of micron sized iron oxide particles in endothelin-1 induced focal cortical ischemia in rats is independent of cell migration</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24788</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Accumulation of micron sized iron oxide particles in endothelin-1 induced focal cortical ischemia in rats is independent of cell migration</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dorit Granot, Erik M. Shapiro</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-09T08:19:52.808394-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24788</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24788</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24788</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24788-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Endogenous labeling of stem/ progenitor cells via intracerebroventricular injection of micron-sized particles of iron oxide (MPIOs) has become standard methodology for MRI of adult neurogenesis. While this method is well characterized in the naïve rodent brain, it has not been fully investigated in disease models. Here, we describe methodological challenges that can confound data analysis when this technique is applied to a rat model of stroke, the endothelin-1 model of focal cortical ischemia.</p></div></div>
<div class="section" id="mrm24788-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>We intended to track endogenous neuroblast migration from the subventricular zone to the stroke area using previously described methods for in vivo labeling of endogenous neuroblasts with MPIOs and following migration with high resolution MRI.</p></div></div>
<div class="section" id="mrm24788-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>MPIOs accumulation in stroke regions of endothelin-1-treated brains involves two dynamic steps: an initial rapid cell independent mechanism, followed by slower MPIOs accumulation. While the latter may in part be attributable to cell dependent delivery of the particles, the cell independent mechanism complicates the interpretation of the data. Strategies aimed at prelabeling the stem cell niche reduced cell independent MPIOs accumulation, but failed to abolish it.</p></div></div>
<div class="section" id="mrm24788-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>We conclude that MRI-based neural stem/progenitor cell tracking via direct injection of MPIOs into the lateral and third ventricles, requires significant validation in models of brain disease/trauma. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Endogenous labeling of stem/ progenitor cells via intracerebroventricular injection of micron-sized particles of iron oxide (MPIOs) has become standard methodology for MRI of adult neurogenesis. While this method is well characterized in the naïve rodent brain, it has not been fully investigated in disease models. Here, we describe methodological challenges that can confound data analysis when this technique is applied to a rat model of stroke, the endothelin-1 model of focal cortical ischemia.


Methods
We intended to track endogenous neuroblast migration from the subventricular zone to the stroke area using previously described methods for in vivo labeling of endogenous neuroblasts with MPIOs and following migration with high resolution MRI.


Results
MPIOs accumulation in stroke regions of endothelin-1-treated brains involves two dynamic steps: an initial rapid cell independent mechanism, followed by slower MPIOs accumulation. While the latter may in part be attributable to cell dependent delivery of the particles, the cell independent mechanism complicates the interpretation of the data. Strategies aimed at prelabeling the stem cell niche reduced cell independent MPIOs accumulation, but failed to abolish it.


Conclusion
We conclude that MRI-based neural stem/progenitor cell tracking via direct injection of MPIOs into the lateral and third ventricles, requires significant validation in models of brain disease/trauma. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24782" xmlns="http://purl.org/rss/1.0/"><title>DCE-MRI analysis methods for predicting the response of breast cancer to neoadjuvant chemotherapy: Pilot study findings</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24782</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">DCE-MRI analysis methods for predicting the response of breast cancer to neoadjuvant chemotherapy: Pilot study findings</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Xia Li, Lori R. Arlinghaus, Gregory D. Ayers, A. Bapsi Chakravarthy, Richard G. Abramson, Vandana G. Abramson, Nkiruka Atuegwu, Jaime Farley, Ingrid A. Mayer, Mark C. Kelley, Ingrid M. Meszoely, Julie Means-Powell, Ana M. Grau, Melinda Sanders, Sandeep R. Bhave, Thomas E. Yankeelov</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-09T08:18:36.402565-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24782</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24782</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24782</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24782-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The purpose of this pilot study is to determine (1) if early changes in both semiquantitative and quantitative DCE-MRI parameters, observed after the first cycle of neoadjuvant chemotherapy in breast cancer patients, show significant difference between responders and nonresponders and (2) if these parameters can be used as a prognostic indicator of the eventual response.</p></div></div>
<div class="section" id="mrm24782-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Twenty-eight patients were examined using DCE-MRI pre-, post-one cycle, and just prior to surgery. The semiquantitative parameters included longest dimension, tumor volume, initial area under the curve, and signal enhancement ratio related parameters, while quantitative parameters included <em>K</em><sup>trans</sup>, <em>v</em><sub><em>e</em></sub>, <em>k</em><sub>ep</sub>, <em>v</em><sub><em>p</em></sub>, and τ<sub><em>i</em></sub> estimated using the standard Tofts-Kety, extended Tofts-Kety, and fast exchange regime models.</p></div></div>
<div class="section" id="mrm24782-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Our preliminary results indicated that the signal enhancement ratio washout volume and <em>k</em><sub>ep</sub> were significantly different between pathologic complete responders from nonresponders (<em>P</em> &lt; 0.05) after a single cycle of chemotherapy. Receiver operator characteristic analysis showed that the AUC of the signal enhancement ratio washout volume was 0.75, and the AUCs of <em>k</em><sub>ep</sub> estimated by three models were 0.78, 0.76, and 0.73, respectively.</p></div></div>
<div class="section" id="mrm24782-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>In summary, the signal enhancement ratio washout volume and <em>k</em><sub>ep</sub> appear to predict breast cancer response after one cycle of neoadjuvant chemotherapy. This observation should be confirmed with additional prospective studies.  Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The purpose of this pilot study is to determine (1) if early changes in both semiquantitative and quantitative DCE-MRI parameters, observed after the first cycle of neoadjuvant chemotherapy in breast cancer patients, show significant difference between responders and nonresponders and (2) if these parameters can be used as a prognostic indicator of the eventual response.


Methods
Twenty-eight patients were examined using DCE-MRI pre-, post-one cycle, and just prior to surgery. The semiquantitative parameters included longest dimension, tumor volume, initial area under the curve, and signal enhancement ratio related parameters, while quantitative parameters included Ktrans, ve, kep, vp, and τi estimated using the standard Tofts-Kety, extended Tofts-Kety, and fast exchange regime models.


Results
Our preliminary results indicated that the signal enhancement ratio washout volume and kep were significantly different between pathologic complete responders from nonresponders (P &lt; 0.05) after a single cycle of chemotherapy. Receiver operator characteristic analysis showed that the AUC of the signal enhancement ratio washout volume was 0.75, and the AUCs of kep estimated by three models were 0.78, 0.76, and 0.73, respectively.


Conclusion
In summary, the signal enhancement ratio washout volume and kep appear to predict breast cancer response after one cycle of neoadjuvant chemotherapy. This observation should be confirmed with additional prospective studies.  Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24778" xmlns="http://purl.org/rss/1.0/"><title>High permittivity pads reduce specific absorption rate, improve B1 homogeneity, and increase contrast-to-noise ratio for functional cardiac MRI at 3 T</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24778</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High permittivity pads reduce specific absorption rate, improve B1 homogeneity, and increase contrast-to-noise ratio for functional cardiac MRI at 3 T</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Wyger M. Brink, Andrew G. Webb</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-09T07:57:04.074783-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24778</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24778</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24778</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24778-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To improve image quality and reduce specific absorption rate in functional cardiac imaging at 3 T.</p></div></div>
<div class="section" id="mrm24652-sec-0018" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Two high permittivity dielectric pads on the anterior and posterior sides of the thorax were numerically designed and implemented using an aqueous suspension of barium titanate. The effects on the average transmit efficiency, B<sub>1</sub> homogeneity, reception sensitivity, and contrast-to-noise ratio were verified in vivo on a dual-transmit system with the body coil driven in conventional quadrature and radiofrequency-shimmed mode.</p></div></div>
<div class="section" id="mrm24652-sec-0019" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Statistically significant improvements in average transmit efficiency, B<sub>1</sub> homogeneity, and contrast-to-noise ratio were measured in healthy volunteers (<em>n</em> = 11) with body mass indices between 20.3 and 34.9. Simulations show that no radiofrequency hot spots are introduced by the dielectric material.</p></div></div>
<div class="section" id="mrm24652-sec-0020" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>High permittivity pads are shown to reduce specific absorption rate, improve B<sub>1</sub> homogeneity, and increase contrast-to-noise ratio in functional cardiac magnetic resonance at 3 T. The results presented in this work show that the current approach is more effective than dual-channel radiofrequency shimming. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To improve image quality and reduce specific absorption rate in functional cardiac imaging at 3 T.


Methods
Two high permittivity dielectric pads on the anterior and posterior sides of the thorax were numerically designed and implemented using an aqueous suspension of barium titanate. The effects on the average transmit efficiency, B1 homogeneity, reception sensitivity, and contrast-to-noise ratio were verified in vivo on a dual-transmit system with the body coil driven in conventional quadrature and radiofrequency-shimmed mode.


Results
Statistically significant improvements in average transmit efficiency, B1 homogeneity, and contrast-to-noise ratio were measured in healthy volunteers (n = 11) with body mass indices between 20.3 and 34.9. Simulations show that no radiofrequency hot spots are introduced by the dielectric material.


Conclusion
High permittivity pads are shown to reduce specific absorption rate, improve B1 homogeneity, and increase contrast-to-noise ratio in functional cardiac magnetic resonance at 3 T. The results presented in this work show that the current approach is more effective than dual-channel radiofrequency shimming. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24731" xmlns="http://purl.org/rss/1.0/"><title>Ultrafast localized two-dimensional magnetic resonance correlated spectroscopy via spatially encoded technique</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24731</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Ultrafast localized two-dimensional magnetic resonance correlated spectroscopy via spatially encoded technique</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yanqin Lin, Qinta Zhang, Zhiliang Wei, Shuhui Cai, Jianhui Zhong, Zhong Chen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-08T07:59:33.795434-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24731</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24731</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24731</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24731-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To speed up acquisition of localized two-dimensional (2D) correlated spectroscopy (LCOSY).</p></div></div>
<div class="section" id="mrm24731-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A new pulse sequence, dubbed as spatially encoded localized COSY (SLCOSY), based on spatially encoded technique, was developed for localized 2D correlated spectroscopy. It can be used to collect a full 2D spectrum in a single scan and thus on a subsecond timescale.</p></div></div>
<div class="section" id="mrm24731-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>SLCOSY spectrum of a two-compartment phantom was obtained with a total acquisition time of 773 ms, with its volume localization confirmed. Localized 2D COSY spectrum of a proton magnetic resonance spectroscopy brain phantom within 12 s shows the ability of SLCOSY to detect the metabolites at physiological concentrations. All 10 constituent metabolites in this phantom are reliably detected. SLCOSY spectrum of a sample of pig brain tissue with the acquisition time of 32 s demonstrates the feasibility of SLCOSY for the detection of biological tissues. Twelve pairs of cross peaks are identified.</p></div></div>
<div class="section" id="mrm24731-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The new method proposed herein enables ultrafast collection of a full 2D COSY spectrum, and it can also be used for fast in vivo analysis of metabolites, when signal-to-noise ratio is not a limiting factor. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To speed up acquisition of localized two-dimensional (2D) correlated spectroscopy (LCOSY).


Methods
A new pulse sequence, dubbed as spatially encoded localized COSY (SLCOSY), based on spatially encoded technique, was developed for localized 2D correlated spectroscopy. It can be used to collect a full 2D spectrum in a single scan and thus on a subsecond timescale.


Results
SLCOSY spectrum of a two-compartment phantom was obtained with a total acquisition time of 773 ms, with its volume localization confirmed. Localized 2D COSY spectrum of a proton magnetic resonance spectroscopy brain phantom within 12 s shows the ability of SLCOSY to detect the metabolites at physiological concentrations. All 10 constituent metabolites in this phantom are reliably detected. SLCOSY spectrum of a sample of pig brain tissue with the acquisition time of 32 s demonstrates the feasibility of SLCOSY for the detection of biological tissues. Twelve pairs of cross peaks are identified.


Conclusion
The new method proposed herein enables ultrafast collection of a full 2D COSY spectrum, and it can also be used for fast in vivo analysis of metabolites, when signal-to-noise ratio is not a limiting factor. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24772" xmlns="http://purl.org/rss/1.0/"><title>Multicenter 
R2* mapping in the healthy brain</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24772</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Multicenter 
R2* mapping in the healthy brain</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Stefan Ropele, Mike P. Wattjes, Christian Langkammer, Iris D. Kilsdonk, Wolter L. Graaf, Jette L Frederiksen, Dan Fuglø, Marios Yiannakas, Claudia A. M. Wheeler-Kingshott, Christian Enzinger, Maria A. Rocca, Till Sprenger, Michael Amman, Ludwig Kappos, Massimo Filippi, Alex Rovira, Olga Ciccarelli, Frederik Barkhof, Franz Fazekas</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-08T07:59:26.342865-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24772</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24772</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24772</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24772-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24772/asset/equation/mrm24772-math-0003.gif?v=1&amp;t=hh1lk3rs&amp;s=4991ea7ed9fc1e206850ea8a86e1f7af4c46cddf" class="inlineGraphic"/> relaxation rate constant has been suggested as a sensitive measure for iron accumulation. The aim of this multi-center study was to assess the inter-scanner and inter-subject variability of 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24772/asset/equation/mrm24772-math-0004.gif?v=1&amp;t=hh1lk3rt&amp;s=7b72f9236b34c384ca06542fd4d269c41d7a09f4" class="inlineGraphic"/> mapping and to investigate the relationship between brain volume and 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24772/asset/equation/mrm24772-math-0005.gif?v=1&amp;t=hh1lk3rt&amp;s=49505d34e0abeb962d836772df795329e87c7cee" class="inlineGraphic"/> in specific structures.</p></div></div>
<div class="section" id="mrm24772-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24772/asset/equation/mrm24772-math-0006.gif?v=1&amp;t=hh1lk3ru&amp;s=1f5e60fdb60638a775df4ebf5616667800049a8c" class="inlineGraphic"/> mapping was performed in 81 healthy subjects in seven centers using different 3 T systems. 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24772/asset/equation/mrm24772-math-0007.gif?v=1&amp;t=hh1lk3ru&amp;s=44232f1204f75198dda2e4d8452037e0fda62504" class="inlineGraphic"/> was calculated from a dual-echo gradient echo sequence and was assessed in several deep gray matter structures. The inter-scanner and inter-subject variability of 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24772/asset/equation/mrm24772-math-0008.gif?v=1&amp;t=hh1lk3rv&amp;s=6dc53fa25e9fe39d66be13f4bed0d3f9879a6c53" class="inlineGraphic"/> was calculated by means of the coefficient of variation before and after correcting for age.</p></div></div>
<div class="section" id="mrm24772-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Significant center effects were seen in some regions which get lost after age correction. The coefficient of variation for the inter-center variability was much lower (&lt;5.6%) than for the intra-subject variability (6.7%–11.7%). 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24772/asset/equation/mrm24772-math-0009.gif?v=1&amp;t=hh1lk3rw&amp;s=62e699f4c4201ca843376c3bb258e9e0bfcc2231" class="inlineGraphic"/> in the putamen and red nucleus scaled with cortical volume while 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24772/asset/equation/mrm24772-math-0010.gif?v=1&amp;t=hh1lk3rw&amp;s=30e2871cca672573c32abb41d44aaed91c9ec67f" class="inlineGraphic"/> in the globus pallidus and the substantia nigra was negatively associated with white matter volume.</p></div></div>
<div class="section" id="mrm24772-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24772/asset/equation/mrm24772-math-0011.gif?v=1&amp;t=hh1lk3rx&amp;s=9c75e9cbeb617d45235f56f1e150ba12481d5cb6" class="inlineGraphic"/> is a robust and reproducible measure in a multicenter setting provided that a standardized MRI protocol is used. The relationship between iron concentration in deep gray matter and volume of specific brain compartments needs further investigation. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The 
R2* relaxation rate constant has been suggested as a sensitive measure for iron accumulation. The aim of this multi-center study was to assess the inter-scanner and inter-subject variability of 
R2* mapping and to investigate the relationship between brain volume and 
R2* in specific structures.


Methods

R2* mapping was performed in 81 healthy subjects in seven centers using different 3 T systems. 
R2* was calculated from a dual-echo gradient echo sequence and was assessed in several deep gray matter structures. The inter-scanner and inter-subject variability of 
R2* was calculated by means of the coefficient of variation before and after correcting for age.


Results
Significant center effects were seen in some regions which get lost after age correction. The coefficient of variation for the inter-center variability was much lower (&lt;5.6%) than for the intra-subject variability (6.7%–11.7%). 
R2* in the putamen and red nucleus scaled with cortical volume while 
R2* in the globus pallidus and the substantia nigra was negatively associated with white matter volume.


Conclusion

R2* is a robust and reproducible measure in a multicenter setting provided that a standardized MRI protocol is used. The relationship between iron concentration in deep gray matter and volume of specific brain compartments needs further investigation. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24774" xmlns="http://purl.org/rss/1.0/"><title>Investigation of resolution effects using a specialized diffusion tensor phantom</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24774</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Investigation of resolution effects using a specialized diffusion tensor phantom</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Michael Bach, Klaus H. Fritzsche, Bram Stieltjes, Frederik B. Laun</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-08T07:59:11.514771-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24774</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24774</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24774</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24774-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The clinical potential of the diffusion imaging-based analysis of fine brain structures such as fornix or cingulum is high due to the central role of these structures in psychiatric diseases. However, the quantification of diffusion parameters in fine structures is especially prone to partial volume effects (PVEs).</p></div></div>
<div class="section" id="mrm24774-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>In this study, a phantom for the investigation of PVEs and their influence on diffusion parameters in fine structures of different diameter is presented. The phantom is produced by winding wet polyester fibers onto a spindle. The resulting fiber strands have well defined square cross-sections of 1–25 mm<sup>2</sup> and provide a homogeneous and high fractional anisotropy (FA ≈ 0.9).</p></div></div>
<div class="section" id="mrm24774-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Several PVEs are demonstrated and analyzed. It is shown that inferred results such as the fiber geometry and diffusion parameters strongly depend on the relative position of the structure of interest to the voxel-grid. Several implications of PVEs on post-processing methods such as Tract-based Spatial Statistics and fiber tractography are demonstrated.</p></div></div>
<div class="section" id="mrm24774-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>These results show that the handling of PVEs in common post-processing tasks can be problematic, and that the presented phantom provides a valuable tool for the improvement and evaluation of these effects. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The clinical potential of the diffusion imaging-based analysis of fine brain structures such as fornix or cingulum is high due to the central role of these structures in psychiatric diseases. However, the quantification of diffusion parameters in fine structures is especially prone to partial volume effects (PVEs).


Methods
In this study, a phantom for the investigation of PVEs and their influence on diffusion parameters in fine structures of different diameter is presented. The phantom is produced by winding wet polyester fibers onto a spindle. The resulting fiber strands have well defined square cross-sections of 1–25 mm2 and provide a homogeneous and high fractional anisotropy (FA ≈ 0.9).


Results
Several PVEs are demonstrated and analyzed. It is shown that inferred results such as the fiber geometry and diffusion parameters strongly depend on the relative position of the structure of interest to the voxel-grid. Several implications of PVEs on post-processing methods such as Tract-based Spatial Statistics and fiber tractography are demonstrated.


Conclusion
These results show that the handling of PVEs in common post-processing tasks can be problematic, and that the presented phantom provides a valuable tool for the improvement and evaluation of these effects. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24775" xmlns="http://purl.org/rss/1.0/"><title>Bone marrow fat quantification in the presence of trabecular bone: Initial comparison between water-fat imaging and single-voxel MRS</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24775</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Bone marrow fat quantification in the presence of trabecular bone: Initial comparison between water-fat imaging and single-voxel MRS</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dimitrios C. Karampinos, Gerd Melkus, Thomas Baum, Jan S. Bauer, Ernst J. Rummeny, Roland Krug</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-08T07:58:42.194078-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24775</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24775</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24775</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24775-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The purpose of the present study was to test the relative performance of chemical shift-based water-fat imaging in measuring bone marrow fat fraction in the presence of trabecular bone, having as reference standard the single-voxel magnetic resonance spectroscopy (MRS).</p></div></div>
<div class="section" id="mrm24775-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Six-echo gradient echo imaging and single-voxel MRS measurements were performed on the proximal femur of seven healthy volunteers. The bone marrow fat spectrum was characterized based on the magnitude of measurable fat peaks and an <em>a priori</em> knowledge of the chemical structure of triglycerides, in order to accurately extract the water peak from the overlapping broad fat peaks in MRS. The imaging-based fat fraction results were then compared to the MRS-based results both without and with taking into consideration the presence of short 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24775/asset/equation/mrm24775-math-0001.gif?v=1&amp;t=hh1lk3s9&amp;s=2ee53cb76ced9b9fb10f0bac951a6f268e25a4e8" class="inlineGraphic"/> water components in MRS.</p></div></div>
<div class="section" id="mrm24775-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>There was a significant underestimation of the fat fraction using the MRS model not accounting for short 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24775/asset/equation/mrm24775-math-0002.gif?v=1&amp;t=hh1lk3sa&amp;s=1c04a7b86a37bc09b8e40275c34b744f2ba7eaf1" class="inlineGraphic"/> species with respect to the imaging-based fat fraction. A good equivalency was observed between the fat fraction using the MRS model accounting for short 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24775/asset/equation/mrm24775-math-0003.gif?v=1&amp;t=hh1lk3sa&amp;s=6316a5a108e238d30ac1a66efa53b9519e61fd5f" class="inlineGraphic"/> species and the imaging-based fat fraction (<em>R</em><sup>2</sup> = 0.87).</p></div></div>
<div class="section" id="mrm24775-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The consideration of the short 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24775/asset/equation/mrm24775-math-0004.gif?v=1&amp;t=hh1lk3sb&amp;s=533ae463d07bc660749d11947de1cfe26382cb1c" class="inlineGraphic"/> water species effect on bone marrow fat quantification is essential when comparing MRS-based and imaging-based fat fraction results. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The purpose of the present study was to test the relative performance of chemical shift-based water-fat imaging in measuring bone marrow fat fraction in the presence of trabecular bone, having as reference standard the single-voxel magnetic resonance spectroscopy (MRS).


Methods
Six-echo gradient echo imaging and single-voxel MRS measurements were performed on the proximal femur of seven healthy volunteers. The bone marrow fat spectrum was characterized based on the magnitude of measurable fat peaks and an a priori knowledge of the chemical structure of triglycerides, in order to accurately extract the water peak from the overlapping broad fat peaks in MRS. The imaging-based fat fraction results were then compared to the MRS-based results both without and with taking into consideration the presence of short 
T2* water components in MRS.


Results
There was a significant underestimation of the fat fraction using the MRS model not accounting for short 
T2* species with respect to the imaging-based fat fraction. A good equivalency was observed between the fat fraction using the MRS model accounting for short 
T2* species and the imaging-based fat fraction (R2 = 0.87).


Conclusion
The consideration of the short 
T2* water species effect on bone marrow fat quantification is essential when comparing MRS-based and imaging-based fat fraction results. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24757" xmlns="http://purl.org/rss/1.0/"><title>Intervertebral disc internal deformation measured by displacements under applied loading with MRI at 3T</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24757</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Intervertebral disc internal deformation measured by displacements under applied loading with MRI at 3T</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Deva D. Chan, Corey P. Neu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-06T07:44:51.095013-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24757</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24757</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24757</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24757-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Noninvasive assessment of tissue mechanical behavior could enable insights into tissue function in healthy and diseased conditions and permit the development of effective tissue repair treatments. Measurement of displacements under applied loading with MRI (dualMRI) has the potential for such biomechanical characterization on a clinical MRI system.</p></div></div>
<div class="section" id="mrm24757-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>dualMRI was translated from high-field research systems to a 3T clinical system. Precision was calculated using repeated tests of a silicone phantom. dualMRI was demonstrated by visualizing displacements and strains in an intervertebral disc and compared to <em>T</em><sub>2</sub> measured during cyclic loading.</p></div></div>
<div class="section" id="mrm24757-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The displacement and strain precisions were 24 µm and 0.3% strain, respectively, under the imaging parameters used in this study. Displacements and strains were measured within the intervertebral disc, but no correlations were found with the <em>T</em><sub>2</sub> values.</p></div></div>
<div class="section" id="mrm24757-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The translation of dualMRI to a 3T system unveils the potential for in vivo studies in a myriad of tissue and organ systems. Because of the importance of mechanical behavior to the function of a variety of tissues, it's expected that dualMRI implemented on a clinical system will be a powerful tool in assessing the interlinked roles of structure, mechanics, and function in both healthy and diseased tissues. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Noninvasive assessment of tissue mechanical behavior could enable insights into tissue function in healthy and diseased conditions and permit the development of effective tissue repair treatments. Measurement of displacements under applied loading with MRI (dualMRI) has the potential for such biomechanical characterization on a clinical MRI system.


Methods
dualMRI was translated from high-field research systems to a 3T clinical system. Precision was calculated using repeated tests of a silicone phantom. dualMRI was demonstrated by visualizing displacements and strains in an intervertebral disc and compared to T2 measured during cyclic loading.


Results
The displacement and strain precisions were 24 µm and 0.3% strain, respectively, under the imaging parameters used in this study. Displacements and strains were measured within the intervertebral disc, but no correlations were found with the T2 values.


Conclusion
The translation of dualMRI to a 3T system unveils the potential for in vivo studies in a myriad of tissue and organ systems. Because of the importance of mechanical behavior to the function of a variety of tissues, it's expected that dualMRI implemented on a clinical system will be a powerful tool in assessing the interlinked roles of structure, mechanics, and function in both healthy and diseased tissues. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24746" xmlns="http://purl.org/rss/1.0/"><title>Comparison of hyperpolarized 3He and 129Xe MRI for the measurement of absolute ventilated lung volume in rats</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24746</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Comparison of hyperpolarized 3He and 129Xe MRI for the measurement of absolute ventilated lung volume in rats</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Matthew S. Fox, Alexei Ouriadov, Giles E. Santyr</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-06T07:44:04.16018-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24746</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24746</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24746</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24746-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>MRI using hyperpolarized noble gases, <sup>3</sup>He and <sup>129</sup>Xe, provides noninvasive assessments of lung structure and function. Previous work demonstrated that absolute ventilated lung volumes (aVLV) measured in rats using hyperpolarized <sup>3</sup>He agree well with micro-CT.</p></div></div>
<div class="section" id="mrm24746-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>In this work, aVLV measurements were performed in rats using hyperpolarized <sup>129</sup>Xe MRI and compared with hyperpolarized <sup>3</sup>He measurements of aVLV under matched ventilation conditions. Whole-lung compliance was also determined. Partial volume, apparent diffusion coefficient, and effective transverse relaxation time corrections were applied during postprocessing to reduce bias between methods.</p></div></div>
<div class="section" id="mrm24746-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Mean apparent diffusion coefficient of the trachea was 0.83 ± 0.09 cm<sup>2</sup>/s and 0.067 ± 0.011 cm<sup>2</sup>/s for <sup>3</sup>He and <sup>129</sup>Xe, respectively. Mean apparent diffusion coefficient of parenchyma was 0.21 ± 0.07 cm<sup>2</sup>/s and 0.027 ± 0.008 cm<sup>2</sup>/s for <sup>3</sup>He and <sup>129</sup>Xe, respectively. Mean transverse relaxation time values were 1.57 ± 0.25 ms and 2.80 ± 0.25 ms for <sup>3</sup>He and <sup>129</sup>Xe, respectively, in a model trachea and 3.18 ± 1.00 ms and 4.88 ± 0.60 ms for <sup>3</sup>He and <sup>129</sup>Xe, respectively, for lung parenchyma. Mean aVLV values were 7.07 ± 0.67 mL and 6.99 ± 1.00 mL at 14 cmH<sub>2</sub>O and 4.88 ± 0.71 mL and 5.36 ± 0.76 mL at 10 cmH<sub>2</sub>O obtained with <sup>3</sup>He and <sup>129</sup>Xe, respectively, demonstrating good agreement between <sup>129</sup>Xe and <sup>3</sup>He.</p></div></div>
<div class="section" id="mrm24746-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p><sup>129</sup>Xe offers an important alternative to <sup>3</sup>He for hyperpolarized gas MRI of aVLV in rats. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
MRI using hyperpolarized noble gases, 3He and 129Xe, provides noninvasive assessments of lung structure and function. Previous work demonstrated that absolute ventilated lung volumes (aVLV) measured in rats using hyperpolarized 3He agree well with micro-CT.


Methods
In this work, aVLV measurements were performed in rats using hyperpolarized 129Xe MRI and compared with hyperpolarized 3He measurements of aVLV under matched ventilation conditions. Whole-lung compliance was also determined. Partial volume, apparent diffusion coefficient, and effective transverse relaxation time corrections were applied during postprocessing to reduce bias between methods.


Results
Mean apparent diffusion coefficient of the trachea was 0.83 ± 0.09 cm2/s and 0.067 ± 0.011 cm2/s for 3He and 129Xe, respectively. Mean apparent diffusion coefficient of parenchyma was 0.21 ± 0.07 cm2/s and 0.027 ± 0.008 cm2/s for 3He and 129Xe, respectively. Mean transverse relaxation time values were 1.57 ± 0.25 ms and 2.80 ± 0.25 ms for 3He and 129Xe, respectively, in a model trachea and 3.18 ± 1.00 ms and 4.88 ± 0.60 ms for 3He and 129Xe, respectively, for lung parenchyma. Mean aVLV values were 7.07 ± 0.67 mL and 6.99 ± 1.00 mL at 14 cmH2O and 4.88 ± 0.71 mL and 5.36 ± 0.76 mL at 10 cmH2O obtained with 3He and 129Xe, respectively, demonstrating good agreement between 129Xe and 3He.


Conclusions
129Xe offers an important alternative to 3He for hyperpolarized gas MRI of aVLV in rats. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24751" xmlns="http://purl.org/rss/1.0/"><title>ESPIRiT—an eigenvalue approach to autocalibrating parallel MRI: Where SENSE meets GRAPPA</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24751</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">ESPIRiT—an eigenvalue approach to autocalibrating parallel MRI: Where SENSE meets GRAPPA</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Martin Uecker, Peng Lai, Mark J. Murphy, Patrick Virtue, Michael Elad, John M. Pauly, Shreyas S. Vasanawala, Michael Lustig</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-06T07:43:27.146933-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24751</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24751</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24751</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24751-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Parallel imaging allows the reconstruction of images from undersampled multicoil data. The two main approaches are: SENSE, which explicitly uses coil sensitivities, and GRAPPA, which makes use of learned correlations in k-space. The purpose of this work is to clarify their relationship and to develop and evaluate an improved algorithm.</p></div></div>
<div class="section" id="mrm24751-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>A theoretical analysis shows: (1) The correlations in k-space are encoded in the null space of a calibration matrix. (2) Both approaches restrict the solution to a subspace spanned by the sensitivities. (3) The sensitivities appear as the main eigenvector of a reconstruction operator computed from the null space. The basic assumptions and the quality of the sensitivity maps are evaluated in experimental examples. The appearance of additional eigenvectors motivates an extended SENSE reconstruction with multiple maps, which is compared to existing methods.</p></div></div>
<div class="section" id="mrm24751-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The existence of a null space and the high quality of the extracted sensitivities are confirmed. The extended reconstruction combines all advantages of SENSE with robustness to certain errors similar to GRAPPA.</p></div></div>
<div class="section" id="mrm24751-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>In this article the gap between both approaches is finally bridged. A new autocalibration technique combines the benefits of both. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Parallel imaging allows the reconstruction of images from undersampled multicoil data. The two main approaches are: SENSE, which explicitly uses coil sensitivities, and GRAPPA, which makes use of learned correlations in k-space. The purpose of this work is to clarify their relationship and to develop and evaluate an improved algorithm.


Theory and Methods
A theoretical analysis shows: (1) The correlations in k-space are encoded in the null space of a calibration matrix. (2) Both approaches restrict the solution to a subspace spanned by the sensitivities. (3) The sensitivities appear as the main eigenvector of a reconstruction operator computed from the null space. The basic assumptions and the quality of the sensitivity maps are evaluated in experimental examples. The appearance of additional eigenvectors motivates an extended SENSE reconstruction with multiple maps, which is compared to existing methods.


Results
The existence of a null space and the high quality of the extracted sensitivities are confirmed. The extended reconstruction combines all advantages of SENSE with robustness to certain errors similar to GRAPPA.


Conclusion
In this article the gap between both approaches is finally bridged. A new autocalibration technique combines the benefits of both. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24761" xmlns="http://purl.org/rss/1.0/"><title>Combined saturation/inversion recovery sequences for improved evaluation of scar and diffuse fibrosis in patients with arrhythmia or heart rate variability</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24761</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Combined saturation/inversion recovery sequences for improved evaluation of scar and diffuse fibrosis in patients with arrhythmia or heart rate variability</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sebastian Weingärtner, Mehmet Akçakaya, Tamer Basha, Kraig V. Kissinger, Beth Goddu, Sophie Berg, Warren J. Manning, Reza Nezafat</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-06T07:42:16.097302-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24761</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24761</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24761</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24761-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To develop arrhythmia-insensitive inversion recovery sequences for improved visualization of myocardial scar and quantification of diffuse fibrosis.</p></div></div>
<div class="section" id="mrm24761-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A novel preparation pre-pulse, called saturation pulse prepared heart-rate-independent inversion recovery, is introduced, which consists of a combination of saturation and inversion pulses to remove the magnetization history in each heartbeat in late gadolinium enhancement (LGE) imaging and eliminate the need for rest periods in <em>T</em><sub>1</sub> mapping. The proposed LGE and <em>T</em><sub>1</sub> mapping sequences were evaluated against conventional LGE and modified Look-Locker inversion sequences using numerical simulations, phantom and imaging in healthy subjects and patients with suspected or known cardiovascular disease.</p></div></div>
<div class="section" id="mrm24761-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Simulations and phantom experiments show that the saturation pulse prepared heart-rate-independent inversion recovery pre-pulse in LGE reduces ghosting artifacts and results in perfect nulling of the healthy myocardium in the presence of arrhythmia. In <em>T</em><sub>1</sub> mapping, saturation pulse prepared heart-rate-independent inversion recovery results in (a) reduced scan time (17 vs. 9 heartbeats), (b) insensitivity to heart rate for long <em>T</em><sub>1</sub>, and (c) increased signal homogeneity for short <em>T</em><sub>1</sub>. LGE images in a patient in atrial fibrillation during the scan show improved myocardial nulling. In vivo <em>T</em><sub>1</sub> maps demonstrate increased signal homogeneity in blood pools and myocardium.</p></div></div>
<div class="section" id="mrm24761-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The proposed sequences are insensitive to heart rate variability, yield improved LGE images in the presence of arrhythmias, as well as <em>T</em><sub>1</sub> mapping with shorter scan times. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To develop arrhythmia-insensitive inversion recovery sequences for improved visualization of myocardial scar and quantification of diffuse fibrosis.


Methods
A novel preparation pre-pulse, called saturation pulse prepared heart-rate-independent inversion recovery, is introduced, which consists of a combination of saturation and inversion pulses to remove the magnetization history in each heartbeat in late gadolinium enhancement (LGE) imaging and eliminate the need for rest periods in T1 mapping. The proposed LGE and T1 mapping sequences were evaluated against conventional LGE and modified Look-Locker inversion sequences using numerical simulations, phantom and imaging in healthy subjects and patients with suspected or known cardiovascular disease.


Results
Simulations and phantom experiments show that the saturation pulse prepared heart-rate-independent inversion recovery pre-pulse in LGE reduces ghosting artifacts and results in perfect nulling of the healthy myocardium in the presence of arrhythmia. In T1 mapping, saturation pulse prepared heart-rate-independent inversion recovery results in (a) reduced scan time (17 vs. 9 heartbeats), (b) insensitivity to heart rate for long T1, and (c) increased signal homogeneity for short T1. LGE images in a patient in atrial fibrillation during the scan show improved myocardial nulling. In vivo T1 maps demonstrate increased signal homogeneity in blood pools and myocardium.


Conclusion
The proposed sequences are insensitive to heart rate variability, yield improved LGE images in the presence of arrhythmias, as well as T1 mapping with shorter scan times. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24754" xmlns="http://purl.org/rss/1.0/"><title>Local field of view imaging for alias-free undersampling with nonlinear spatial encoding magnetic fields</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24754</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Local field of view imaging for alias-free undersampling with nonlinear spatial encoding magnetic fields</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hans Weber, Gerrit Schultz, Daniel Gallichan, Jürgen Hennig, Maxim Zaitsev</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-03T08:12:18.247892-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24754</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24754</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24754</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24754-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Nonlinear spatial encoding magnetic fields result in an inhomogeneous image resolution. Within this study, this characteristic property of nonlinear encoding is investigated with regard to its potential to accelerate MRI acquisitions.</p></div></div>
<div class="section" id="mrm24754-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory</h4><div class="para"><p>A dependency between k-space coverage and local resolvability of the image causes k-space samples to have a spatially localized contribution to the reconstruction of the spin density. On the basis of this observation, a concept for alias-free data undersampling is developed, which is referred to as the local field of view concept.</p></div></div>
<div class="section" id="mrm24754-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>On the basis of this concept, a fast sampling trajectory is developed. It is evaluated with simulations and experiments (both using a phantom and in vivo) for MRI with, as an example, pure quadrupolar encoding fields. To demonstrate that the concept is only applicable to (spatially) nonlinear encoding, a comparison with linear encoding is provided.</p></div></div>
<div class="section" id="mrm24754-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Application of the local field of view concept results in a localized adaptation of the image resolution by undersampling higher frequency k-space samples without introducing aliasing.</p></div></div>
<div class="section" id="mrm24754-sec-0050" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>A new effect of nonlinear spatial encoding magnetic fields was found, which allows more efficient data sampling and at the same time counterbalancing the natural variation in image resolution. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Nonlinear spatial encoding magnetic fields result in an inhomogeneous image resolution. Within this study, this characteristic property of nonlinear encoding is investigated with regard to its potential to accelerate MRI acquisitions.


Theory
A dependency between k-space coverage and local resolvability of the image causes k-space samples to have a spatially localized contribution to the reconstruction of the spin density. On the basis of this observation, a concept for alias-free data undersampling is developed, which is referred to as the local field of view concept.


Methods
On the basis of this concept, a fast sampling trajectory is developed. It is evaluated with simulations and experiments (both using a phantom and in vivo) for MRI with, as an example, pure quadrupolar encoding fields. To demonstrate that the concept is only applicable to (spatially) nonlinear encoding, a comparison with linear encoding is provided.


Results
Application of the local field of view concept results in a localized adaptation of the image resolution by undersampling higher frequency k-space samples without introducing aliasing.


Conclusions
A new effect of nonlinear spatial encoding magnetic fields was found, which allows more efficient data sampling and at the same time counterbalancing the natural variation in image resolution. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24768" xmlns="http://purl.org/rss/1.0/"><title>In vivo imaging of islet transplantation using PLGA nanoparticles containing iron oxide and indocyanine green</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24768</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">In vivo imaging of islet transplantation using PLGA nanoparticles containing iron oxide and indocyanine green</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jung Hwan Hwang, Young-Woock Noh, Jung-Hyun Choi, Jung-Ran Noh, Yong-Hoon Kim, Gil-Tae Gang, Kyoung-Shim Kim, Hye Sun Park, Yong Taik Lim, Hyeyoung Moon, Kwan Soo Hong, Hee Gu Lee, Bong Hyun Chung, Chul-Ho Lee</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-02T08:18:15.678035-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24768</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24768</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24768</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24768-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>We determined whether poly(lactic-<em>co</em>-glycolic acid) nanoparticles would be a useful reagent for the successful monitoring of isolated islets by magnetic resonance imaging and optical imaging systems, without clinically relevant toxicity in vitro or in vivo.</p></div></div>
<div class="section" id="mrm24768-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>We used iron oxide for MR imaging and a cyanide dye approved by the Food and Drug Administration (indocyanine green) for optical imaging and estimated the in vivo detection of transplanted pancreatic islets.</p></div></div>
<div class="section" id="mrm24768-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The poly(lactic-<em>co</em>-glycolic acid) nanoparticles were associated with the islets in vitro and were successfully detected by 4.7 T (MR) and optical imaging, without other toxic effects. When labeled islets were transplanted under the mouse kidney capsule, in vivo <em>T</em><sub>2</sub><em>/</em>
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24768/asset/equation/mrm24768-math-0001.gif?v=1&amp;t=hh1lk3tb&amp;s=abc9bfe0addd39ba87fdf33091576f848b346b03" class="inlineGraphic"/>-weighted scans with 4.7 T MR detected as few as 300 labeled islets by 4 weeks. Optical in vivo imaging revealed indocyanine green fluorescence by 2 and 4 days after transplantation of islets containing 250 and 500 µg/mL poly(lactic-<em>co</em>-glycolic acid) nanoparticles, respectively. These results were further supported by the immunohistochemical results for insulin and iron in the recipient mouse kidney and pancreas.</p></div></div>
<div class="section" id="mrm24768-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>Taken together, these data indicate that poly(lactic-<em>co</em>-glycolic acid) nanoparticles may be used to label transplanted islets and may be imaged with in vivo MR and optical imaging systems. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
We determined whether poly(lactic-co-glycolic acid) nanoparticles would be a useful reagent for the successful monitoring of isolated islets by magnetic resonance imaging and optical imaging systems, without clinically relevant toxicity in vitro or in vivo.


Methods
We used iron oxide for MR imaging and a cyanide dye approved by the Food and Drug Administration (indocyanine green) for optical imaging and estimated the in vivo detection of transplanted pancreatic islets.


Results
The poly(lactic-co-glycolic acid) nanoparticles were associated with the islets in vitro and were successfully detected by 4.7 T (MR) and optical imaging, without other toxic effects. When labeled islets were transplanted under the mouse kidney capsule, in vivo T2/
T2*-weighted scans with 4.7 T MR detected as few as 300 labeled islets by 4 weeks. Optical in vivo imaging revealed indocyanine green fluorescence by 2 and 4 days after transplantation of islets containing 250 and 500 µg/mL poly(lactic-co-glycolic acid) nanoparticles, respectively. These results were further supported by the immunohistochemical results for insulin and iron in the recipient mouse kidney and pancreas.


Conclusions
Taken together, these data indicate that poly(lactic-co-glycolic acid) nanoparticles may be used to label transplanted islets and may be imaged with in vivo MR and optical imaging systems. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24763" xmlns="http://purl.org/rss/1.0/"><title>Detection of in vivo enzyme activity with CatalyCEST MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24763</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Detection of in vivo enzyme activity with CatalyCEST MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Byunghee Yoo, Vipul R. Sheth, Christine M. Howison, Matthew J. K. Douglas, Carlos T. Pineda, Erin A. Maine, Amanda F. Baker, Mark D. Pagel</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-02T08:17:58.927538-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24763</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24763</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24763</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24763-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>CatalyCEST MRI compares the detection of an enzyme-responsive chemical exchange saturation transfer (CEST) agent with the detection of an unresponsive “control” CEST agent that accounts for other conditions that influence CEST. The purpose of this study was to investigate the feasibility of in vivo catalyCEST MRI.</p></div></div>
<div class="section" id="mrm24763-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>CEST agents that were responsive and unresponsive to the activity of urokinase plasminogen activator were shown to have negligible interaction with each other. A CEST-fast imaging with steady state precession (FISP) MRI protocol was used to acquire MR CEST spectroscopic images with a Capan-2 pancreatic tumor model after intravenous injection of the CEST agents. A function of (super)-Lorentzian line shapes was fit to CEST spectra of a region-of-interest that represented the tumor.</p></div></div>
<div class="section" id="mrm24763-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The CEST effects from each agent showed the same initial uptake into tumor tissues, indicating that both agents had the same pharmacokinetic transport rates. Starting 5 min after injection, CEST from the enzyme-responsive agent disappeared more quickly than CEST from the unresponsive agent, indicating that the enzyme responsive agent was being catalyzed by urokinase plasminogen activator, while both agents also experienced net pharmacokinetic washout from the tumor.</p></div></div>
<div class="section" id="mrm24763-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>CatalyCEST MRI demonstrates that dynamic tracking of enzyme-responsive and unresponsive CEST agents during the same in vivo MRI study is feasible. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
CatalyCEST MRI compares the detection of an enzyme-responsive chemical exchange saturation transfer (CEST) agent with the detection of an unresponsive “control” CEST agent that accounts for other conditions that influence CEST. The purpose of this study was to investigate the feasibility of in vivo catalyCEST MRI.


Methods
CEST agents that were responsive and unresponsive to the activity of urokinase plasminogen activator were shown to have negligible interaction with each other. A CEST-fast imaging with steady state precession (FISP) MRI protocol was used to acquire MR CEST spectroscopic images with a Capan-2 pancreatic tumor model after intravenous injection of the CEST agents. A function of (super)-Lorentzian line shapes was fit to CEST spectra of a region-of-interest that represented the tumor.


Results
The CEST effects from each agent showed the same initial uptake into tumor tissues, indicating that both agents had the same pharmacokinetic transport rates. Starting 5 min after injection, CEST from the enzyme-responsive agent disappeared more quickly than CEST from the unresponsive agent, indicating that the enzyme responsive agent was being catalyzed by urokinase plasminogen activator, while both agents also experienced net pharmacokinetic washout from the tumor.


Conclusion
CatalyCEST MRI demonstrates that dynamic tracking of enzyme-responsive and unresponsive CEST agents during the same in vivo MRI study is feasible. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24749" xmlns="http://purl.org/rss/1.0/"><title>Cerebral TOF angiography at 7T: Impact of B1+ shimming with a 16-channel transceiver array</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24749</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cerebral TOF angiography at 7T: Impact of B1+ shimming with a 16-channel transceiver array</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sebastian Schmitter, Xiaoping Wu, Gregor Adriany, Edward J. Auerbach, Kâmil Uğurbil, Pierre-François Moortele</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-02T08:15:25.564452-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24749</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24749</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24749</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24749-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Time-of-flight (TOF) MR imaging is clinically among the most common cerebral noncontrast enhanced MR angiography techniques allowing for high spatial resolution. As shown by several groups TOF contrast significantly improves at ultrahigh field of <em>B</em><sub>0</sub> = 7T, however, spatially varying transmit <em>B</em><sub>1</sub> (<em>B</em><sub>1</sub><sup>+</sup>) fields at 7T reduce TOF contrast uniformity, typically resulting in suboptimal contrast and reduced vessel conspicuity in the brain periphery.</p></div></div>
<div class="section" id="mrm24749-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Using a 16-channel <em>B</em><sub>1</sub><sup>+</sup> shimming system, we compare different dynamically applied <em>B</em><sub>1</sub><sup>+</sup> phase shimming approaches on the radiofrequency excitation to improve contrast homogeneity for a (0.5 mm)<sup>3</sup> resolution multislab TOF acquisition. In addition, <em>B</em><sub>1</sub><sup>+</sup> shimming applied on the venous saturation pulse was investigated to improve venous suppression, subcutaneous fat signal reduction and enhanced background suppression originating from MT effect.</p></div></div>
<div class="section" id="mrm24749-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p><em>B</em><sub>1</sub><em><sup>+</sup></em> excitation homogeneity was improved by a factor 2.2–2.6 on average depending on the shimming approach, compared to a standard CP-like phase setting, leading to improved vessel conspicuity particularly in the periphery. Stronger saturation, higher fat suppression and improved background suppression were observed when dynamically applying <em>B</em><sub>1</sub><sup>+</sup> shimming on the venous saturation pulse.</p></div></div>
<div class="section" id="mrm24749-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p><em>B</em><sub>1</sub><em>+</em> shimming can significantly improve high resolution TOF vascular investigations at ultrahigh field, holding strong promise for non contrast-enhanced clinical applications. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Time-of-flight (TOF) MR imaging is clinically among the most common cerebral noncontrast enhanced MR angiography techniques allowing for high spatial resolution. As shown by several groups TOF contrast significantly improves at ultrahigh field of B0 = 7T, however, spatially varying transmit B1 (B1+) fields at 7T reduce TOF contrast uniformity, typically resulting in suboptimal contrast and reduced vessel conspicuity in the brain periphery.


Methods
Using a 16-channel B1+ shimming system, we compare different dynamically applied B1+ phase shimming approaches on the radiofrequency excitation to improve contrast homogeneity for a (0.5 mm)3 resolution multislab TOF acquisition. In addition, B1+ shimming applied on the venous saturation pulse was investigated to improve venous suppression, subcutaneous fat signal reduction and enhanced background suppression originating from MT effect.


Results
B1+ excitation homogeneity was improved by a factor 2.2–2.6 on average depending on the shimming approach, compared to a standard CP-like phase setting, leading to improved vessel conspicuity particularly in the periphery. Stronger saturation, higher fat suppression and improved background suppression were observed when dynamically applying B1+ shimming on the venous saturation pulse.


Conclusion
B1+ shimming can significantly improve high resolution TOF vascular investigations at ultrahigh field, holding strong promise for non contrast-enhanced clinical applications. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24762" xmlns="http://purl.org/rss/1.0/"><title>Magnetic susceptibility induced white matter MR signal frequency shifts—experimental comparison between Lorentzian sphere and generalized Lorentzian approaches</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24762</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Magnetic susceptibility induced white matter MR signal frequency shifts—experimental comparison between Lorentzian sphere and generalized Lorentzian approaches</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">J. Luo, X. He, D. A. Yablonskiy</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-01T14:29:11.223501-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24762</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24762</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24762</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24762-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The nature of the remarkable phase contrast in high-field gradient echo MRI studies of human brain is a subject of intense debates. The generalized Lorentzian approach (He and Yablonskiy, Proc Natl Acad Sci USA 2009;106:13558–13563) provides an explanation for the anisotropy of phase contrast, the near absence of phase contrast between white matter and cerebrospinal fluid, and changes of phase contrast in multiple sclerosis. In this study, we experimentally validate the generalized Lorentzian approach.</p></div></div>
<div class="section" id="mrm24762-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>The Generalized Lorentzian Approach suggests that the local contribution to frequency shifts in white matter does not depend on the average tissue magnetic susceptibility (as suggested by Lorentzian sphere approximation), but on the distribution and symmetry of magnetic susceptibility inclusions at the cellular level. We use ex vivo rat optic nerve as a model system of highly organized cellular structure containing longitudinally arranged myelin and neurofilaments. The nerve's cylindrical shape allowed accurate measurement of its magnetic susceptibility and local frequency shifts.</p></div></div>
<div class="section" id="mrm24762-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>We found that the volume magnetic susceptibility difference between nerve and water is −0.116 ppm, and the magnetic susceptibilities of longitudinal components are −0.043 ppm in fresh nerve, and −0.020 ppm in fixed nerve.</p></div></div>
<div class="section" id="mrm24762-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The frequency shift observed in the optic nerve as a representative of white matter is consistent with generalized Lorentzian approach but inconsistent with Lorentzian sphere approximation. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The nature of the remarkable phase contrast in high-field gradient echo MRI studies of human brain is a subject of intense debates. The generalized Lorentzian approach (He and Yablonskiy, Proc Natl Acad Sci USA 2009;106:13558–13563) provides an explanation for the anisotropy of phase contrast, the near absence of phase contrast between white matter and cerebrospinal fluid, and changes of phase contrast in multiple sclerosis. In this study, we experimentally validate the generalized Lorentzian approach.


Theory and Methods
The Generalized Lorentzian Approach suggests that the local contribution to frequency shifts in white matter does not depend on the average tissue magnetic susceptibility (as suggested by Lorentzian sphere approximation), but on the distribution and symmetry of magnetic susceptibility inclusions at the cellular level. We use ex vivo rat optic nerve as a model system of highly organized cellular structure containing longitudinally arranged myelin and neurofilaments. The nerve's cylindrical shape allowed accurate measurement of its magnetic susceptibility and local frequency shifts.


Results
We found that the volume magnetic susceptibility difference between nerve and water is −0.116 ppm, and the magnetic susceptibilities of longitudinal components are −0.043 ppm in fresh nerve, and −0.020 ppm in fixed nerve.


Conclusion
The frequency shift observed in the optic nerve as a representative of white matter is consistent with generalized Lorentzian approach but inconsistent with Lorentzian sphere approximation. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24764" xmlns="http://purl.org/rss/1.0/"><title>Variable flip angle balanced steady-state free precession for lower SAR or higher contrast cardiac cine imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24764</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Variable flip angle balanced steady-state free precession for lower SAR or higher contrast cardiac cine imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Subashini Srinivasan, Daniel B. Ennis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-29T14:20:36.80347-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24764</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24764</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24764</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24764-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Cardiac cine balanced steady-state free precession (bSSFP) imaging uses a high flip angle (FA) to obtain high blood-myocardium signal-to-noise and contrast-to-noise ratios (CNR). Use of high FAs, however, results in substantially increased SAR. Our objective was to develop a variable FA bSSFP cardiac cine imaging technique with: (1) low SAR and blood-myocardium CNR similar to conventional constant FA bSSFP (CFA-bSSFP) or (2) increased blood-myocardium CNR compared to CFA-bSSFP with similar SAR.</p></div></div>
<div class="section" id="mrm24764-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Variable FA bSSFP cardiac cine imaging was achieved using an asynchronous k-space acquisition, which is asynchronous to the cardiac cycle (aVFA-bSSFP). Bloch simulations and phantom experiments were performed to compare the signal, resolution, and frequency response of the variable FA bSSFP and CFA-bSSFP schemes. Ten volunteers were imaged with different aVFA-bSSFP and asynchronous CFA-bSSFP schemes and compared to conventional segmented CFA-bSSFP.</p></div></div>
<div class="section" id="mrm24764-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The SAR of aVFA-bSSFP is significantly decreased by 36% compared to asynchronous CFA-bSSFP (1.9 ± 0.2 vs. 3.0 ± 0.2 W/kg, <em>P</em> &lt;  10<sup>−10</sup>) for similar blood-myocardium CNR (34 ± 6 vs. 35 ± 9, <em>P</em> = 0.5). Alternately, the CNR of the aVFA-bSSFP is improved by 28% compared to asynchronous CFA-bSSFP (49 ± 9 vs. 38 ± 8, <em>P</em> &lt;  10<sup>−4</sup>) with similar SAR (3.2 ± 0.5 vs. 3.3 ± 0.5 W/kg, <em>P</em> = 0.6).</p></div></div>
<div class="section" id="mrm24764-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>aVFA-bSSFP can be used for lower SAR or higher contrast cardiac cine imaging compared to the conventional segmented CFA-bSSFP imaging. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Cardiac cine balanced steady-state free precession (bSSFP) imaging uses a high flip angle (FA) to obtain high blood-myocardium signal-to-noise and contrast-to-noise ratios (CNR). Use of high FAs, however, results in substantially increased SAR. Our objective was to develop a variable FA bSSFP cardiac cine imaging technique with: (1) low SAR and blood-myocardium CNR similar to conventional constant FA bSSFP (CFA-bSSFP) or (2) increased blood-myocardium CNR compared to CFA-bSSFP with similar SAR.


Methods
Variable FA bSSFP cardiac cine imaging was achieved using an asynchronous k-space acquisition, which is asynchronous to the cardiac cycle (aVFA-bSSFP). Bloch simulations and phantom experiments were performed to compare the signal, resolution, and frequency response of the variable FA bSSFP and CFA-bSSFP schemes. Ten volunteers were imaged with different aVFA-bSSFP and asynchronous CFA-bSSFP schemes and compared to conventional segmented CFA-bSSFP.


Results
The SAR of aVFA-bSSFP is significantly decreased by 36% compared to asynchronous CFA-bSSFP (1.9 ± 0.2 vs. 3.0 ± 0.2 W/kg, P &lt;  10−10) for similar blood-myocardium CNR (34 ± 6 vs. 35 ± 9, P = 0.5). Alternately, the CNR of the aVFA-bSSFP is improved by 28% compared to asynchronous CFA-bSSFP (49 ± 9 vs. 38 ± 8, P &lt;  10−4) with similar SAR (3.2 ± 0.5 vs. 3.3 ± 0.5 W/kg, P = 0.6).


Conclusion
aVFA-bSSFP can be used for lower SAR or higher contrast cardiac cine imaging compared to the conventional segmented CFA-bSSFP imaging. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24766" xmlns="http://purl.org/rss/1.0/"><title>Integrated parallel reception, excitation, and shimming (iPRES)</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24766</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Integrated parallel reception, excitation, and shimming (iPRES)</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hui Han, Allen W. Song, Trong-Kha Truong</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-29T14:20:21.756669-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24766</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24766</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24766</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Rapid Communication</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24766-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To develop a new concept for a hardware platform that enables integrated parallel reception, excitation, and shimming (iPRES).</p></div></div>
<div class="section" id="mrm24766-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory</h4><div class="para"><p>This concept uses a single coil array rather than separate arrays for parallel excitation/reception and <em>B</em><sub>0</sub> shimming. It relies on a novel design that allows a radiofrequency current (for excitation/reception) and a direct current (for <em>B</em><sub>0</sub> shimming) to coexist independently in the same coil.</p></div></div>
<div class="section" id="mrm24766-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Proof-of-concept <em>B</em><sub>0</sub> shimming experiments were performed with a two-coil array in a phantom, whereas <em>B</em><sub>0</sub> shimming simulations were performed with a 48-coil array in the human brain.</p></div></div>
<div class="section" id="mrm24766-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Our experiments show that individually optimized direct currents applied in each coil can reduce the <em>B</em><sub>0</sub> root-mean-square error by 62–81% and minimize distortions in echo-planar images. The simulations show that dynamic shimming with the 48-coil iPRES array can reduce the <em>B</em><sub>0</sub> root-mean-square error in the prefrontal and temporal regions by 66–79% as compared with static second-order spherical harmonic shimming and by 12–23% as compared with dynamic shimming with a 48-coil conventional shim array.</p></div></div>
<div class="section" id="mrm24766-sec-0005" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Our results demonstrate the feasibility of the iPRES concept to perform parallel excitation/reception and <em>B</em><sub>0</sub> shimming with a unified coil system as well as its promise for in vivo applications. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To develop a new concept for a hardware platform that enables integrated parallel reception, excitation, and shimming (iPRES).


Theory
This concept uses a single coil array rather than separate arrays for parallel excitation/reception and B0 shimming. It relies on a novel design that allows a radiofrequency current (for excitation/reception) and a direct current (for B0 shimming) to coexist independently in the same coil.


Methods
Proof-of-concept B0 shimming experiments were performed with a two-coil array in a phantom, whereas B0 shimming simulations were performed with a 48-coil array in the human brain.


Results
Our experiments show that individually optimized direct currents applied in each coil can reduce the B0 root-mean-square error by 62–81% and minimize distortions in echo-planar images. The simulations show that dynamic shimming with the 48-coil iPRES array can reduce the B0 root-mean-square error in the prefrontal and temporal regions by 66–79% as compared with static second-order spherical harmonic shimming and by 12–23% as compared with dynamic shimming with a 48-coil conventional shim array.


Conclusion
Our results demonstrate the feasibility of the iPRES concept to perform parallel excitation/reception and B0 shimming with a unified coil system as well as its promise for in vivo applications. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24767" xmlns="http://purl.org/rss/1.0/"><title>Dynamic and inherent B0 correction for DTI using stimulated echo spiral imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24767</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Dynamic and inherent B0 correction for DTI using stimulated echo spiral imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Alexandru V. Avram, Arnaud Guidon, Trong-Kha Truong, Chunlei Liu, Allen W. Song</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-29T14:19:57.423327-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24767</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24767</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24767</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24767-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To present a novel technique for high-resolution stimulated echo diffusion tensor imaging with self-navigated interleaved spirals readout trajectories that can inherently and dynamically correct for image artifacts due to spatial and temporal variations in the static magnetic field (<em>B</em><sub>0</sub>) resulting from eddy currents, tissue susceptibilities, subject/physiological motion, and hardware instabilities.</p></div></div>
<div class="section" id="mrm24767-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The Hahn spin echo formed by the first two 90° radiofrequency pulses is balanced to consecutively acquire two additional images with different echo times and generate an inherent field map, while the diffusion-prepared stimulated echo signal remains unaffected. For every diffusion-encoding direction, an intrinsically registered field map is estimated dynamically and used to effectively and inherently correct for off-resonance artifacts in the reconstruction of the corresponding diffusion-weighted image.</p></div></div>
<div class="section" id="mrm24767-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>After correction with the dynamically acquired field maps, local blurring artifacts are specifically removed from individual stimulated echo diffusion-weighted images and the estimated diffusion tensors have significantly improved spatial accuracy and larger fractional anisotropy.</p></div></div>
<div class="section" id="mrm24767-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Combined with the self-navigated interleaved spirals acquisition scheme, our new method provides an integrated high-resolution short-echo time diffusion tensor imaging solution with inherent and dynamic correction for both motion-induced phase errors and off-resonance effects. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To present a novel technique for high-resolution stimulated echo diffusion tensor imaging with self-navigated interleaved spirals readout trajectories that can inherently and dynamically correct for image artifacts due to spatial and temporal variations in the static magnetic field (B0) resulting from eddy currents, tissue susceptibilities, subject/physiological motion, and hardware instabilities.


Methods
The Hahn spin echo formed by the first two 90° radiofrequency pulses is balanced to consecutively acquire two additional images with different echo times and generate an inherent field map, while the diffusion-prepared stimulated echo signal remains unaffected. For every diffusion-encoding direction, an intrinsically registered field map is estimated dynamically and used to effectively and inherently correct for off-resonance artifacts in the reconstruction of the corresponding diffusion-weighted image.


Results
After correction with the dynamically acquired field maps, local blurring artifacts are specifically removed from individual stimulated echo diffusion-weighted images and the estimated diffusion tensors have significantly improved spatial accuracy and larger fractional anisotropy.


Conclusion
Combined with the self-navigated interleaved spirals acquisition scheme, our new method provides an integrated high-resolution short-echo time diffusion tensor imaging solution with inherent and dynamic correction for both motion-induced phase errors and off-resonance effects. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24769" xmlns="http://purl.org/rss/1.0/"><title>Ultrashort echo time bi-component analysis of cortical bone—a field dependence study</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24769</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Ultrashort echo time bi-component analysis of cortical bone—a field dependence study</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Shihong Li, Eric Y. Chang, Won C. Bae, Christine B. Chung, Song Gao, Shanglian Bao, Graeme M. Bydder, Yanqing Hua, Jiang Du</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-29T14:19:46.056459-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24769</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24769</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24769</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24769-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The purpose of this study is to investigate the effect of differing field strength on the 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24769/asset/equation/mrm24769-math-0001.gif?v=1&amp;t=hh1lk3vs&amp;s=12477c381e8a84e304c1d802e461ec35b313144b" class="inlineGraphic"/> of cortical bone at 1.5 T and 3 T.</p></div></div>
<div class="section" id="mrm24769-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Ultrashort echo time pulse sequences were used to study six bovine and nine human bone samples at 1.5 T and 3 T using single- and bi-component 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24769/asset/equation/mrm24769-math-0002.gif?v=1&amp;t=hh1lk3vt&amp;s=e9d44c71032cc8da3788f2a19d3919a4713aea3e" class="inlineGraphic"/> analysis.</p></div></div>
<div class="section" id="mrm24769-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>On average, the bound water 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24769/asset/equation/mrm24769-math-0003.gif?v=1&amp;t=hh1lk3vu&amp;s=24d7c4334f60b928dce2337d6403c194d42500d3" class="inlineGraphic"/> of bovine bone decreased by 16% (from 0.32 ms at 1.5 T to 0.27 ms at 3 T, <em>P</em> &lt; 0.01) and the bound water 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24769/asset/equation/mrm24769-math-0004.gif?v=1&amp;t=hh1lk3vu&amp;s=62922bd6034aef59c3abe20df781b228be5acf38" class="inlineGraphic"/> of human bone decreased by 21% (from 0.42 ms at 1.5 T to 0.33 ms at 3 T, <em>P</em> &lt; 0.01) at the higher field strength. The free water 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24769/asset/equation/mrm24769-math-0005.gif?v=1&amp;t=hh1lk3vv&amp;s=1367eb8d31a1cb6495150ddce920ec162124fae2" class="inlineGraphic"/> of bovine bone decreased by 50% (from 4.23 ms at 1.5 T to 2.12 ms at 3 T, <em>P</em> &lt; 0.001) and the free water 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24769/asset/equation/mrm24769-math-0006.gif?v=1&amp;t=hh1lk3vv&amp;s=eea9f9118e5b9f7b0305f1acdae5dca561267850" class="inlineGraphic"/> of human bone decreased by 68% (from 7.65 ms at 1.5 T to 2.46 ms at 3 T, <em>P</em> &lt; 0.001) at the higher field strength. Bound and free water fractions showed only minor change with field strength in bovine (&lt; 2%, <em>P</em> &gt; 0.05) and human bone (&lt; 4%, <em>P</em> &gt; 0.05).</p></div></div>
<div class="section" id="mrm24769-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Ultrashort echo time bi-component analysis provides consistent bound and free water fractions at 1.5 T and 3 T, thereby allowing field-independent comparisons. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The purpose of this study is to investigate the effect of differing field strength on the 
T2* of cortical bone at 1.5 T and 3 T.


Methods
Ultrashort echo time pulse sequences were used to study six bovine and nine human bone samples at 1.5 T and 3 T using single- and bi-component 
T2* analysis.


Results
On average, the bound water 
T2* of bovine bone decreased by 16% (from 0.32 ms at 1.5 T to 0.27 ms at 3 T, P &lt; 0.01) and the bound water 
T2* of human bone decreased by 21% (from 0.42 ms at 1.5 T to 0.33 ms at 3 T, P &lt; 0.01) at the higher field strength. The free water 
T2* of bovine bone decreased by 50% (from 4.23 ms at 1.5 T to 2.12 ms at 3 T, P &lt; 0.001) and the free water 
T2* of human bone decreased by 68% (from 7.65 ms at 1.5 T to 2.46 ms at 3 T, P &lt; 0.001) at the higher field strength. Bound and free water fractions showed only minor change with field strength in bovine (&lt; 2%, P &gt; 0.05) and human bone (&lt; 4%, P &gt; 0.05).


Conclusion
Ultrashort echo time bi-component analysis provides consistent bound and free water fractions at 1.5 T and 3 T, thereby allowing field-independent comparisons. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24736" xmlns="http://purl.org/rss/1.0/"><title>Design of multishell sampling schemes with uniform coverage in diffusion MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24736</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Design of multishell sampling schemes with uniform coverage in diffusion MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Emmanuel Caruyer, Christophe Lenglet, Guillermo Sapiro, Rachid Deriche</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T08:20:49.373444-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24736</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24736</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24736</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Rapid Communication</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24736-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>In diffusion MRI, a technique known as diffusion spectrum imaging reconstructs the propagator with a discrete Fourier transform, from a Cartesian sampling of the diffusion signal. Alternatively, it is possible to directly reconstruct the orientation distribution function in <em>q</em>-ball imaging, providing so-called high angular resolution diffusion imaging. In between these two techniques, acquisitions on several spheres in q-space offer an interesting trade-off between the angular resolution and the radial information gathered in diffusion MRI. A careful design is central in the success of multishell acquisition and reconstruction techniques.</p></div></div>
<div class="section" id="mrm24736-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The design of acquisition in multishell is still an open and active field of research, however. In this work, we provide a general method to design multishell acquisition with uniform angular coverage. This method is based on a generalization of electrostatic repulsion to multishell.</p></div></div>
<div class="section" id="mrm24736-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>We evaluate the impact of our method using simulations, on the angular resolution in one and two bundles of fiber configurations. Compared to more commonly used radial sampling, we show that our method improves the angular resolution, as well as fiber crossing discrimination.</p></div></div>
<div class="section" id="mrm24736-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Discussion</h4><div class="para"><p>We propose a novel method to design sampling schemes with optimal angular coverage and show the positive impact on angular resolution in diffusion MRI. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
In diffusion MRI, a technique known as diffusion spectrum imaging reconstructs the propagator with a discrete Fourier transform, from a Cartesian sampling of the diffusion signal. Alternatively, it is possible to directly reconstruct the orientation distribution function in q-ball imaging, providing so-called high angular resolution diffusion imaging. In between these two techniques, acquisitions on several spheres in q-space offer an interesting trade-off between the angular resolution and the radial information gathered in diffusion MRI. A careful design is central in the success of multishell acquisition and reconstruction techniques.


Methods
The design of acquisition in multishell is still an open and active field of research, however. In this work, we provide a general method to design multishell acquisition with uniform angular coverage. This method is based on a generalization of electrostatic repulsion to multishell.


Results
We evaluate the impact of our method using simulations, on the angular resolution in one and two bundles of fiber configurations. Compared to more commonly used radial sampling, we show that our method improves the angular resolution, as well as fiber crossing discrimination.


Discussion
We propose a novel method to design sampling schemes with optimal angular coverage and show the positive impact on angular resolution in diffusion MRI. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24759" xmlns="http://purl.org/rss/1.0/"><title>Simultaneous imaging of in vivo conductivity and susceptibility</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24759</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Simultaneous imaging of in vivo conductivity and susceptibility</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dong-Hyun Kim, Narae Choi, Sung-Min Gho, Jaewook Shin, Chunlei Liu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T13:49:11.793659-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24759</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24759</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24759</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24759-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Approaches for quantitative mapping of electric conductivity and magnetic susceptibility using MRI have been developed independently. The purpose of this study is to present a method to simultaneously acquire information on conductivity and susceptibility and to produce images based on these properties.</p></div></div>
<div class="section" id="mrm24759-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A 3D multiecho gradient-echo sequence was used. Phase evolution during the multiecho was used to produce quantitative susceptibility maps, while the phase value at zero echo time was retrieved, and used to generates quantitative conductivity maps. Electromagnetic simulations were performed to evaluate the phase distribution due to conductivity variations. Phantom and in vivo data were also acquired to assess the quality of images produced.</p></div></div>
<div class="section" id="mrm24759-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Simulations demonstrated that phase differences across objects increase<span class="struck ">s</span> with size and conductivity. For an accurate conductivity estimate, the maximum echo time was approximately equal to the true 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24759/asset/equation/mrm24759-math-0001.gif?v=1&amp;t=hh1lk3w5&amp;s=e933ae440d6d0762a42236d2c773a12bc1959562" class="inlineGraphic"/> value in order to achieve signal-to-noise ratio maximization. The most accurate susceptibility was obtained when separating phase contribution from conductivity. Phantom and in vivo results showed good quality images representing the electromagnetic properties.</p></div></div>
<div class="section" id="mrm24759-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>A simultaneous quantitative electromagnetic property imaging approach is demonstrated here. The approach not only improves the efficiency of mapping electromagnetic properties, but can also improve the accuracy of susceptibility mapping by separating image phases introduced by conductivity and susceptibility. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Approaches for quantitative mapping of electric conductivity and magnetic susceptibility using MRI have been developed independently. The purpose of this study is to present a method to simultaneously acquire information on conductivity and susceptibility and to produce images based on these properties.


Methods
A 3D multiecho gradient-echo sequence was used. Phase evolution during the multiecho was used to produce quantitative susceptibility maps, while the phase value at zero echo time was retrieved, and used to generates quantitative conductivity maps. Electromagnetic simulations were performed to evaluate the phase distribution due to conductivity variations. Phantom and in vivo data were also acquired to assess the quality of images produced.


Results
Simulations demonstrated that phase differences across objects increases with size and conductivity. For an accurate conductivity estimate, the maximum echo time was approximately equal to the true 
T2* value in order to achieve signal-to-noise ratio maximization. The most accurate susceptibility was obtained when separating phase contribution from conductivity. Phantom and in vivo results showed good quality images representing the electromagnetic properties.


Conclusion
A simultaneous quantitative electromagnetic property imaging approach is demonstrated here. The approach not only improves the efficiency of mapping electromagnetic properties, but can also improve the accuracy of susceptibility mapping by separating image phases introduced by conductivity and susceptibility. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24760" xmlns="http://purl.org/rss/1.0/"><title>Quantitative MRI analysis of menisci using biexponential T2* fitting with a variable echo time sequence</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24760</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Quantitative MRI analysis of menisci using biexponential T2* fitting with a variable echo time sequence</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mag Vladimir Juras, Sebastian Apprich, Mag. Štefan Zbýň, Lukas Zak, Xeni Deligianni, Pavol Szomolanyi, Oliver Bieri, Siegfried Trattnig</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T13:49:04.369237-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24760</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24760</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24760</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24760-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The goal of this study was to differentiate between normal, degenerative meniscus, and meniscal tears using monoexponentially and biexponentially calculated <em>T</em><sub>2</sub>*. Meniscal disease, characterized by an altered collagen fiber matrix, might be detectable in vivo using quantitative <em>T</em><sub>2</sub>* mapping.</p></div></div>
<div class="section" id="mrm24760-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A 3D Cartesian spoiled gradient echo technique was adapted to enable the use of a variable echo time approach in combination with a highly asymmetric readout. <em>T</em><sub>2</sub>* was calculated monoexponentially and biexponentially using three- and five-parametric non-linear fits, respectively.</p></div></div>
<div class="section" id="mrm24760-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>From a total of 68 evaluated menisci, 48 were normal, 12 were degenerated, and eight had tears. Mean values for the short (<em>T</em><sub>2</sub>*<sub>s</sub>) and long (<em>T</em><sub>2</sub>*<sub>l</sub>) <em>T</em><sub>2</sub>* components were as follows: in normal menisci, 0.82 ± 0.38/15.0 ± 5.4 ms, respectively; in degenerated menisci, 1.29 ± 0.53/19.97 ± 5.59 ms, respectively; and, in meniscal tears, 2.05 ± 0.73 and 26.83 ± 7.72 ms, respectively. Biexponentially fitted <em>T</em><sub>2</sub>* demonstrated a greater ability to distinguish normal and degenerated menisci using receiver operating characteristic (ROC) analysis (higher area under curve as well as higher specificity and sensitivity).</p></div></div>
<div class="section" id="mrm24760-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>This study suggests that biexponential fitting, used for <em>T</em><sub>2</sub>* calculation in the menisci, provides better results compared to monoexponential fitting. Observed changes in <em>T</em><sub>2</sub>* result from the matrix reorganization in degenerative processes in the menisci, which affects the collagen fiber orientation, as well as content. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc</b>.</p></div></div>
]]></content:encoded><description>

Purpose
The goal of this study was to differentiate between normal, degenerative meniscus, and meniscal tears using monoexponentially and biexponentially calculated T2*. Meniscal disease, characterized by an altered collagen fiber matrix, might be detectable in vivo using quantitative T2* mapping.


Methods
A 3D Cartesian spoiled gradient echo technique was adapted to enable the use of a variable echo time approach in combination with a highly asymmetric readout. T2* was calculated monoexponentially and biexponentially using three- and five-parametric non-linear fits, respectively.


Results
From a total of 68 evaluated menisci, 48 were normal, 12 were degenerated, and eight had tears. Mean values for the short (T2*s) and long (T2*l) T2* components were as follows: in normal menisci, 0.82 ± 0.38/15.0 ± 5.4 ms, respectively; in degenerated menisci, 1.29 ± 0.53/19.97 ± 5.59 ms, respectively; and, in meniscal tears, 2.05 ± 0.73 and 26.83 ± 7.72 ms, respectively. Biexponentially fitted T2* demonstrated a greater ability to distinguish normal and degenerated menisci using receiver operating characteristic (ROC) analysis (higher area under curve as well as higher specificity and sensitivity).


Conclusion
This study suggests that biexponential fitting, used for T2* calculation in the menisci, provides better results compared to monoexponential fitting. Observed changes in T2* result from the matrix reorganization in degenerative processes in the menisci, which affects the collagen fiber orientation, as well as content. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24758" xmlns="http://purl.org/rss/1.0/"><title>Improved respiratory efficiency of 3D late gadolinium enhancement imaging using the continuously adaptive windowing strategy (CLAWS)</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24758</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Improved respiratory efficiency of 3D late gadolinium enhancement imaging using the continuously adaptive windowing strategy (CLAWS)</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jennifer Keegan, Permi Jhooti, Sonya V Babu-Narayan, Peter Drivas, Sabine Ernst, David N. Firmin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T13:48:56.792704-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24758</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24758</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24758</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24758-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Acquisition durations of navigator-gated high-resolution three-dimensional late gadolinium enhancement studies may typically be up to 10 min, depending on the respiratory efficiency and heart rate. Implementation of the continuously adaptive windowing strategy (CLAWS) could increase respiratory efficiency, but the resulting non-smooth k-space acquisition order during gadolinium wash-out could result in increased artifact.</p></div></div>
<div class="section" id="mrm24758-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Navigator-gated three-dimensional late gadolinium enhancement acquisitions were performed in 18 patients using tracking end-expiratory accept/reject (EE-ARA) and CLAWS algorithms in random order.</p></div></div>
<div class="section" id="mrm24758-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Retrospective analysis of the stored navigator data shows that CLAWS scan times are very close to (within 1%) or equal to the fastest achievable scan times while EE-ARA significantly extends the acquisition duration (<em>P</em> &lt; 0.0001). EE-ARA acquisitions are 26% longer than CLAWS acquisitions (378 ± 104 s compared to 301 ± 85 s, <em>P</em> = 0.002). Image quality scores for CLAWS and EE-ARA acquisitions are not significantly different (4.1 ± 0.6 compared to 4.3 ± 0.6, <em>P</em> = ns). Numerical phantom simulations show that the non-uniform k-space ordering introduced by CLAWS results in slight, but not statistically significant, reductions in both blood signal-to-noise ratio (10%) and blood-myocardium contrast-to-noise ratio (12%).</p></div></div>
<div class="section" id="mrm24758-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>CLAWS results in markedly reduced acquisition durations compared to EE-ARA without significant detriment to the image quality. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc</b>.</p></div></div>
]]></content:encoded><description>

Purpose
Acquisition durations of navigator-gated high-resolution three-dimensional late gadolinium enhancement studies may typically be up to 10 min, depending on the respiratory efficiency and heart rate. Implementation of the continuously adaptive windowing strategy (CLAWS) could increase respiratory efficiency, but the resulting non-smooth k-space acquisition order during gadolinium wash-out could result in increased artifact.


Methods
Navigator-gated three-dimensional late gadolinium enhancement acquisitions were performed in 18 patients using tracking end-expiratory accept/reject (EE-ARA) and CLAWS algorithms in random order.


Results
Retrospective analysis of the stored navigator data shows that CLAWS scan times are very close to (within 1%) or equal to the fastest achievable scan times while EE-ARA significantly extends the acquisition duration (P &lt; 0.0001). EE-ARA acquisitions are 26% longer than CLAWS acquisitions (378 ± 104 s compared to 301 ± 85 s, P = 0.002). Image quality scores for CLAWS and EE-ARA acquisitions are not significantly different (4.1 ± 0.6 compared to 4.3 ± 0.6, P = ns). Numerical phantom simulations show that the non-uniform k-space ordering introduced by CLAWS results in slight, but not statistically significant, reductions in both blood signal-to-noise ratio (10%) and blood-myocardium contrast-to-noise ratio (12%).


Conclusions
CLAWS results in markedly reduced acquisition durations compared to EE-ARA without significant detriment to the image quality. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24756" xmlns="http://purl.org/rss/1.0/"><title>Fast magnetization transfer and apparent T1 imaging using a short saturation pulse with and without inversion preparation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24756</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Fast magnetization transfer and apparent T1 imaging using a short saturation pulse with and without inversion preparation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tae Kim, Wanyong Shin, Seong-Gi Kim</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T13:48:51.518113-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24756</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24756</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24756</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24756-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Measurements of magnetization transfer (MT) metrics, such as the steady-state (SS) MT ratio and apparent longitudinal relaxation rate require multiple MT irradiation durations and a long experimental time. To overcome these problems, we propose a novel method using a short MT off-resonance pulse with and without on-resonance inversion preparation pulse.</p></div></div>
<div class="section" id="mrm24756-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>Computer simulations were performed to examine the accuracy of the proposed method and to find the optimal off-resonance irradiation pulse duration (<em>T</em><sub>irad</sub>) and power level (<em>ω</em><sub>1</sub>). Our approach, with echo planar imaging data acquisition, was applied to animals at 9.4 T and humans at 3 T with <em>ω</em><sub>1</sub>/2π = 100 Hz and 177 Hz, respectively. Steady-state MT ratio and relaxation rate were obtained from a pair of MT images at a <em>T</em><sub>irad</sub>, with and without inversion.</p></div></div>
<div class="section" id="mrm24756-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>For <em>T</em><sub>irad</sub> ≥ 0.4 s, steady-state MT ratio, and relaxation rate measured at any single <em>T</em><sub>irad</sub> agreed well with those of the conventional fitting method that uses multiple <em>T</em><sub>irad</sub>. Our simulation indicates that a higher <em>ω</em><sub>1</sub> can use a shorter Tirad.</p></div></div>
<div class="section" id="mrm24756-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Steady-state MT ratio and relaxation rate can be determined from MT data with only one, short <em>T</em><sub>irad</sub> by incorporation of an inversion prepulse. This MT imaging approach is simple, fast, and easily implementable. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc</b>.</p></div></div>
]]></content:encoded><description>

Purpose
Measurements of magnetization transfer (MT) metrics, such as the steady-state (SS) MT ratio and apparent longitudinal relaxation rate require multiple MT irradiation durations and a long experimental time. To overcome these problems, we propose a novel method using a short MT off-resonance pulse with and without on-resonance inversion preparation pulse.


Theory and Methods
Computer simulations were performed to examine the accuracy of the proposed method and to find the optimal off-resonance irradiation pulse duration (Tirad) and power level (ω1). Our approach, with echo planar imaging data acquisition, was applied to animals at 9.4 T and humans at 3 T with ω1/2π = 100 Hz and 177 Hz, respectively. Steady-state MT ratio and relaxation rate were obtained from a pair of MT images at a Tirad, with and without inversion.


Results
For Tirad ≥ 0.4 s, steady-state MT ratio, and relaxation rate measured at any single Tirad agreed well with those of the conventional fitting method that uses multiple Tirad. Our simulation indicates that a higher ω1 can use a shorter Tirad.


Conclusion
Steady-state MT ratio and relaxation rate can be determined from MT data with only one, short Tirad by incorporation of an inversion prepulse. This MT imaging approach is simple, fast, and easily implementable. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24732" xmlns="http://purl.org/rss/1.0/"><title>Two-dimensional J-resolved LASER and semi-LASER spectroscopy of human brain</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24732</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Two-dimensional J-resolved LASER and semi-LASER spectroscopy of human brain</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Meijin Lin, Anand Kumar, Shaolin Yang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-19T13:48:44.292467-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24732</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24732</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24732</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24732-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Two-dimensional J-resolved localized and semi-localized by adiabatic selective refocusing (LASER and semi-LASER) spectroscopy, named “J-resolved LASER” and “J-resolved semi-LASER”, were introduced to suppress chemical shift artifacts, additional J-refocused artifactual peaks from spatially dependent J-coupling evolution, and sensitivity to radiofrequency (RF) field inhomogeneity.</p></div></div>
<div class="section" id="mrm24732-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Three pairs of adiabatic pulses were employed for voxel localization in J-resolved LASER and two pairs in J-resolved semi-LASER. The first half of <em>t</em><sub>1</sub> period was inserted between the last pair of adiabatic pulses, which was proposed in this work to obtain two-dimensional adiabatic J-resolved spectra of human brain for the first time. Phantom and human experiments were performed to demonstrate their feasibility and advantages over conventional J-resolved spectroscopy (JPRESS).</p></div></div>
<div class="section" id="mrm24732-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Compared to JPRESS, J-resolved LASER or J-resolved semi-LASER exhibited significant suppression of chemical shift artifacts and additional J-refocused peaks from spatially dependent J-coupling evolution, and demonstrated insensitivity to the change of RF frequency offset over large bandwidth.</p></div></div>
<div class="section" id="mrm24732-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Experiments on phantoms and human brains verified the feasibility and strengths of two-dimensional adiabatic J-resolved spectroscopy at 3T. This technique is expected to advance the application of in vivo two-dimensional MR spectroscopy at 3T and higher field strengths for more reliable and accurate quantification of metabolites. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc</b>.</p></div></div>
]]></content:encoded><description>

Purpose
Two-dimensional J-resolved localized and semi-localized by adiabatic selective refocusing (LASER and semi-LASER) spectroscopy, named “J-resolved LASER” and “J-resolved semi-LASER”, were introduced to suppress chemical shift artifacts, additional J-refocused artifactual peaks from spatially dependent J-coupling evolution, and sensitivity to radiofrequency (RF) field inhomogeneity.


Methods
Three pairs of adiabatic pulses were employed for voxel localization in J-resolved LASER and two pairs in J-resolved semi-LASER. The first half of t1 period was inserted between the last pair of adiabatic pulses, which was proposed in this work to obtain two-dimensional adiabatic J-resolved spectra of human brain for the first time. Phantom and human experiments were performed to demonstrate their feasibility and advantages over conventional J-resolved spectroscopy (JPRESS).


Results
Compared to JPRESS, J-resolved LASER or J-resolved semi-LASER exhibited significant suppression of chemical shift artifacts and additional J-refocused peaks from spatially dependent J-coupling evolution, and demonstrated insensitivity to the change of RF frequency offset over large bandwidth.


Conclusion
Experiments on phantoms and human brains verified the feasibility and strengths of two-dimensional adiabatic J-resolved spectroscopy at 3T. This technique is expected to advance the application of in vivo two-dimensional MR spectroscopy at 3T and higher field strengths for more reliable and accurate quantification of metabolites. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24743" xmlns="http://purl.org/rss/1.0/"><title>Experimentally and computationally fast method for estimation of a mean kurtosis</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24743</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Experimentally and computationally fast method for estimation of a mean kurtosis</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Brian Hansen, Torben E. Lund, Ryan Sangill, Sune Nørhøj Jespersen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-15T10:40:43.289322-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24743</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24743</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24743</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Rapid Communication</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24743-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Results from several recent studies suggest the magnetic resonance diffusion-derived metric mean kurtosis (MK) to be a sensitive marker for tissue pathology; however, lengthy acquisition and postprocessing time hamper further exploration. The purpose of this study is to introduce and evaluate a new MK metric and a rapid protocol for its estimation.</p></div></div>
<div class="section" id="mrm24743-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The protocol requires acquisition of 13 standard diffusion-weighted images, followed by linear combination of log diffusion signals, thus avoiding nonlinear optimization. The method was evaluated on an ex vivo rat brain and an in vivo human brain. Parameter maps were compared with MK estimated from a standard diffusion kurtosis imaging (DKI) data set comprising 160 diffusion-weighted images.</p></div></div>
<div class="section" id="mrm24743-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The new MK displays remarkably similar contrast to MK, and the proposed protocol acquires the necessary data in less than 1 min for full human brain coverage, with a postprocessing time of a few seconds. Scan–rescan reproducibility was comparable with MK.</p></div></div>
<div class="section" id="mrm24743-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The framework offers a robust and rapid method for estimating MK, with a protocol easily adapted on commercial scanners, as it requires only minimal modification of standard diffusion-weighting protocols. These properties make the method feasible in practically any clinical setting. <b>Magn Reson Med 000:000–000, 2013. © 2013 Wiley Periodicals, Inc</b>.</p></div></div>
]]></content:encoded><description>

Purpose
Results from several recent studies suggest the magnetic resonance diffusion-derived metric mean kurtosis (MK) to be a sensitive marker for tissue pathology; however, lengthy acquisition and postprocessing time hamper further exploration. The purpose of this study is to introduce and evaluate a new MK metric and a rapid protocol for its estimation.


Methods
The protocol requires acquisition of 13 standard diffusion-weighted images, followed by linear combination of log diffusion signals, thus avoiding nonlinear optimization. The method was evaluated on an ex vivo rat brain and an in vivo human brain. Parameter maps were compared with MK estimated from a standard diffusion kurtosis imaging (DKI) data set comprising 160 diffusion-weighted images.


Results
The new MK displays remarkably similar contrast to MK, and the proposed protocol acquires the necessary data in less than 1 min for full human brain coverage, with a postprocessing time of a few seconds. Scan–rescan reproducibility was comparable with MK.


Conclusion
The framework offers a robust and rapid method for estimating MK, with a protocol easily adapted on commercial scanners, as it requires only minimal modification of standard diffusion-weighting protocols. These properties make the method feasible in practically any clinical setting. Magn Reson Med 000:000–000, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24744" xmlns="http://purl.org/rss/1.0/"><title>A 1.5T MRI-conditional 12-lead electrocardiogram for MRI and intra-MR intervention</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24744</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A 1.5T MRI-conditional 12-lead electrocardiogram for MRI and intra-MR intervention</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zion Tsz Ho Tse, Charles L. Dumoulin, Gari D. Clifford, Jeff Schweitzer, Lei Qin, Julien Oster, Michael Jerosch-Herold, Raymond Y. Kwong, Gregory Michaud, William G. Stevenson, Ehud J. Schmidt</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-11T08:43:11.182295-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24744</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24744</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24744</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24744-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>High-fidelity 12-lead electrocardiogram (ECG) is important for physiological monitoring of patients during MR-guided intervention and cardiac MRI. Issues in obtaining noncorrupted ECGs inside MRI include a superimposed magneto-hydro-dynamic voltage, gradient switching-induced voltages, and radiofrequency heating. These problems increase with magnetic field. The aim of this study is to develop and clinically validate a 1.5T MRI-conditional 12-lead ECG system.</p></div></div>
<div class="section" id="mrm24744-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The system was constructed including transmission lines to reduce radiofrequency induction and switching circuits to remove induced voltages. Adaptive filters, trained by 12-lead measurements outside MRI and in two orientations inside MRI, were used to remove magneto-hydro-dynamic voltage. The system was tested on 10 (one exercising) volunteers and four arrhythmia patients.</p></div></div>
<div class="section" id="mrm24744-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Switching circuits removed most imaging-induced voltages (residual noise &lt;3% of the R-wave). Magneto-hydro-dynamic voltage removal provided intra-MRI ECGs that varied by &lt;3.8% from those outside the MRI, preserving the true S-wave to T-wave segment. In premature ventricular contraction (PVC) patients, clean ECGs separated premature ventricular contraction and sinus rhythm beats. Measured heating was &lt;1.5°C. The system reliably acquired multiphase (steady-state free precession) wall-motion-cine and phase-contrast-cine scans, including subjects in whom 4-lead gating failed. The system required a minimum repetition time of 4 ms to allow robust ECG processing.</p></div></div>
<div class="section" id="mrm24744-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>High-fidelity intra-MRI 12-lead ECG is possible. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
High-fidelity 12-lead electrocardiogram (ECG) is important for physiological monitoring of patients during MR-guided intervention and cardiac MRI. Issues in obtaining noncorrupted ECGs inside MRI include a superimposed magneto-hydro-dynamic voltage, gradient switching-induced voltages, and radiofrequency heating. These problems increase with magnetic field. The aim of this study is to develop and clinically validate a 1.5T MRI-conditional 12-lead ECG system.


Methods
The system was constructed including transmission lines to reduce radiofrequency induction and switching circuits to remove induced voltages. Adaptive filters, trained by 12-lead measurements outside MRI and in two orientations inside MRI, were used to remove magneto-hydro-dynamic voltage. The system was tested on 10 (one exercising) volunteers and four arrhythmia patients.


Results
Switching circuits removed most imaging-induced voltages (residual noise &lt;3% of the R-wave). Magneto-hydro-dynamic voltage removal provided intra-MRI ECGs that varied by &lt;3.8% from those outside the MRI, preserving the true S-wave to T-wave segment. In premature ventricular contraction (PVC) patients, clean ECGs separated premature ventricular contraction and sinus rhythm beats. Measured heating was &lt;1.5°C. The system reliably acquired multiphase (steady-state free precession) wall-motion-cine and phase-contrast-cine scans, including subjects in whom 4-lead gating failed. The system required a minimum repetition time of 4 ms to allow robust ECG processing.


Conclusion
High-fidelity intra-MRI 12-lead ECG is possible. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24742" xmlns="http://purl.org/rss/1.0/"><title>Voltage-based device tracking in a 1.5 tesla MRI during imaging: initial validation in swine models</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24742</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Voltage-based device tracking in a 1.5 tesla MRI during imaging: initial validation in swine models</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ehud J. Schmidt, Zion T. H. Tse, Tobias R. Reichlin, Gregory F. Michaud, Ronald D. Watkins, Kim Butts-Pauly, Raymond Y. Kwong, William Stevenson, Jeffrey Schweitzer, Israel Byrd, Charles L. Dumoulin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-11T08:42:01.904238-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24742</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24742</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24742</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24742-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Voltage-based device-tracking (VDT) systems are commonly used for tracking invasive devices in electrophysiological cardiac-arrhythmia therapy. During electrophysiological procedures, electro-anatomic mapping workstations provide guidance by integrating VDT location and intracardiac electrocardiogram information with X-ray, computerized tomography, ultrasound, and MR images. MR assists navigation, mapping, and radiofrequency ablation. Multimodality interventions require multiple patient transfers between an MRI and the X-ray/ultrasound electrophysiological suite, increasing the likelihood of patient-motion and image misregistration. An MRI-compatible VDT system may increase efficiency, as there is currently no single method to track devices both inside and outside the MRI scanner.</p></div></div>
<div class="section" id="mrm24742-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>An MRI-compatible VDT system was constructed by modifying a commercial system. Hardware was added to reduce MRI gradient-ramp and radiofrequency unblanking pulse interference. VDT patches and cables were modified to reduce heating. Five swine cardiac VDT electro-anatomic mapping interventions were performed, navigating inside and thereafter outside the MRI.</p></div></div>
<div class="section" id="mrm24742-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Three-catheter VDT interventions were performed at &gt;12 frames per second both inside and outside the MRI scanner with &lt;3 mm error. Catheters were followed on VDT- and MRI-derived maps. Simultaneous VDT and imaging was possible in repetition time &gt;32 ms sequences with &lt;0.5 mm errors, and &lt;5% MRI signal-to-noise ratio (SNR) loss. At shorter repetition times, only intracardiac electrocardiogram was reliable. Radiofrequency heating was &lt;1.5°C.</p></div></div>
<div class="section" id="mrm24742-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>An MRI-compatible VDT system is feasible. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Voltage-based device-tracking (VDT) systems are commonly used for tracking invasive devices in electrophysiological cardiac-arrhythmia therapy. During electrophysiological procedures, electro-anatomic mapping workstations provide guidance by integrating VDT location and intracardiac electrocardiogram information with X-ray, computerized tomography, ultrasound, and MR images. MR assists navigation, mapping, and radiofrequency ablation. Multimodality interventions require multiple patient transfers between an MRI and the X-ray/ultrasound electrophysiological suite, increasing the likelihood of patient-motion and image misregistration. An MRI-compatible VDT system may increase efficiency, as there is currently no single method to track devices both inside and outside the MRI scanner.


Methods
An MRI-compatible VDT system was constructed by modifying a commercial system. Hardware was added to reduce MRI gradient-ramp and radiofrequency unblanking pulse interference. VDT patches and cables were modified to reduce heating. Five swine cardiac VDT electro-anatomic mapping interventions were performed, navigating inside and thereafter outside the MRI.


Results
Three-catheter VDT interventions were performed at &gt;12 frames per second both inside and outside the MRI scanner with &lt;3 mm error. Catheters were followed on VDT- and MRI-derived maps. Simultaneous VDT and imaging was possible in repetition time &gt;32 ms sequences with &lt;0.5 mm errors, and &lt;5% MRI signal-to-noise ratio (SNR) loss. At shorter repetition times, only intracardiac electrocardiogram was reliable. Radiofrequency heating was &lt;1.5°C.


Conclusion
An MRI-compatible VDT system is feasible. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24728" xmlns="http://purl.org/rss/1.0/"><title>Denoising diffusion-weighted magnitude MR images using rank and edge constraints</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24728</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Denoising diffusion-weighted magnitude MR images using rank and edge constraints</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Fan Lam, S. Derin Babacan, Justin P. Haldar, Michael W. Weiner, Norbert Schuff, Zhi-Pei Liang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T11:15:58.906018-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24728</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24728</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24728</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24728-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To improve signal-to-noise ratio for diffusion-weighted magnetic resonance images.</p></div></div>
<div class="section" id="mrm24728-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A new method is proposed for denoising diffusion-weighted magnitude images. The proposed method formulates the denoising problem as an maximum a posteriori} estimation problem based on Rician/noncentral χ likelihood models, incorporating an edge prior and a low-rank model. The resulting optimization problem is solved efficiently using a half-quadratic method with an alternating minimization scheme.</p></div></div>
<div class="section" id="mrm24728-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The performance of the proposed method has been validated using simulated and experimental data. Diffusion-weighted images and noisy data were simulated based on the diffusion tensor imaging model and Rician/noncentral χ distributions. The simulation study (with known gold standard) shows substantial improvements in single-to-noise ratio and diffusion tensor estimation after denoising. In vivo diffusion imaging data at different <em>b</em>-values were acquired. Based on the experimental data, qualitative improvement in image quality and quantitative improvement in diffusion tensor estimation were demonstrated. Additionally, the proposed method is shown to outperform one of the state-of-the-art nonlocal means-based denoising algorithms, both qualitatively and quantitatively.</p></div></div>
<div class="section" id="mrm24728-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The single-to-noise ratio of diffusion-weighted images can be effectively improved with rank and edge constraints, resulting in an improvement in diffusion parameter estimation accuracy.</p></div></div>
]]></content:encoded><description>

Purpose
To improve signal-to-noise ratio for diffusion-weighted magnetic resonance images.


Methods
A new method is proposed for denoising diffusion-weighted magnitude images. The proposed method formulates the denoising problem as an maximum a posteriori} estimation problem based on Rician/noncentral χ likelihood models, incorporating an edge prior and a low-rank model. The resulting optimization problem is solved efficiently using a half-quadratic method with an alternating minimization scheme.


Results
The performance of the proposed method has been validated using simulated and experimental data. Diffusion-weighted images and noisy data were simulated based on the diffusion tensor imaging model and Rician/noncentral χ distributions. The simulation study (with known gold standard) shows substantial improvements in single-to-noise ratio and diffusion tensor estimation after denoising. In vivo diffusion imaging data at different b-values were acquired. Based on the experimental data, qualitative improvement in image quality and quantitative improvement in diffusion tensor estimation were demonstrated. Additionally, the proposed method is shown to outperform one of the state-of-the-art nonlocal means-based denoising algorithms, both qualitatively and quantitatively.


Conclusion
The single-to-noise ratio of diffusion-weighted images can be effectively improved with rank and edge constraints, resulting in an improvement in diffusion parameter estimation accuracy.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24750" xmlns="http://purl.org/rss/1.0/"><title>Vessel-specific quantification of blood oxygenation with T2-relaxation-under-phase-contrast MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24750</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Vessel-specific quantification of blood oxygenation with T2-relaxation-under-phase-contrast MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lisa C. Krishnamurthy, Peiying Liu, Yulin Ge, Hanzhang Lu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T08:11:35.477616-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24750</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24750</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24750</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24750-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Measurement of venous oxygenation (<em>Y</em><sub>v</sub>) is a critical step toward quantitative assessment of brain oxygen metabolism, a key index in many brain disorders. The present study aims to develop a noninvasive, rapid, and reproducible method to measure <em>Y</em><sub>v</sub> in a vessel-specific manner.</p></div></div>
<div class="section" id="mrm24750-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory</h4><div class="para"><p>The method, <em>T</em><sub>2</sub>-Relaxation-Under-Phase-Contrast MRI, utilizes complex subtraction of phase-contrast to isolate pure blood signal, applies nonslice-selective <em>T</em><sub>2</sub>-preparation to measure <em>T</em><sub>2</sub>, and converts <em>T</em><sub>2</sub> to oxygenation using a calibration plot.</p></div></div>
<div class="section" id="mrm24750-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Following feasibility demonstration, several technical aspects were examined, including validation with an established global <em>Y</em><sub>v</sub> technique, test–retest reproducibility, sensitivity to detect oxygenation changes due to hypoxia and caffeine challenges, applicability of echo-planar-imaging (EPI) acquisition to shorten scan duration, and ability to study veins with a caliber of 1–2 mm.</p></div></div>
<div class="section" id="mrm24750-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p><em>T</em><sub>2</sub>-Relaxation-Under-Phase-Contrast was able to simultaneously measure <em>Y</em><sub>v</sub> in all major veins in the brain, including sagittal sinus, straight sinus, great vein, and internal cerebral vein. <em>T</em><sub>2</sub>-Relaxation-Under-Phase-Contrast results showed an excellent agreement with the reference technique, high sensitivity to oxygenation changes, and test–retest variability of 3.5 ± 1.0%. The use of segmented-EPI was able to reduce the scan duration to 1.5 minutes. It was also feasible to study pial veins and deep veins.</p></div></div>
<div class="section" id="mrm24750-sec-0005" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p><em>T</em><sub>2</sub>-Relaxation-Under-Phase-Contrast MRI is a promising technique for vessel-specific oxygenation measurement. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Measurement of venous oxygenation (Yv) is a critical step toward quantitative assessment of brain oxygen metabolism, a key index in many brain disorders. The present study aims to develop a noninvasive, rapid, and reproducible method to measure Yv in a vessel-specific manner.


Theory
The method, T2-Relaxation-Under-Phase-Contrast MRI, utilizes complex subtraction of phase-contrast to isolate pure blood signal, applies nonslice-selective T2-preparation to measure T2, and converts T2 to oxygenation using a calibration plot.


Methods
Following feasibility demonstration, several technical aspects were examined, including validation with an established global Yv technique, test–retest reproducibility, sensitivity to detect oxygenation changes due to hypoxia and caffeine challenges, applicability of echo-planar-imaging (EPI) acquisition to shorten scan duration, and ability to study veins with a caliber of 1–2 mm.


Results
T2-Relaxation-Under-Phase-Contrast was able to simultaneously measure Yv in all major veins in the brain, including sagittal sinus, straight sinus, great vein, and internal cerebral vein. T2-Relaxation-Under-Phase-Contrast results showed an excellent agreement with the reference technique, high sensitivity to oxygenation changes, and test–retest variability of 3.5 ± 1.0%. The use of segmented-EPI was able to reduce the scan duration to 1.5 minutes. It was also feasible to study pial veins and deep veins.


Conclusion
T2-Relaxation-Under-Phase-Contrast MRI is a promising technique for vessel-specific oxygenation measurement. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24741" xmlns="http://purl.org/rss/1.0/"><title>Clinically viable magnetic poly(lactide-co-glycolide) particles for MRI-based cell tracking</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24741</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Clinically viable magnetic poly(lactide-co-glycolide) particles for MRI-based cell tracking</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dorit Granot, Michael K. Nkansah, Margaret F. Bennewitz, Kevin S. Tang, Eleni A. Markakis, Erik M. Shapiro</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T08:11:18.376797-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24741</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24741</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24741</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24741-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To design, fabricate, characterize, and in vivo assay clinically viable magnetic particles for MRI-based cell tracking.</p></div></div>
<div class="section" id="mrm24741-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Poly(lactide-<em>co</em>-glycolide) (PLGA) encapsulated magnetic nano and microparticles were fabricated. Multiple biologically relevant experiments were performed to assess cell viability, cellular performance, and stem cell differentiation. In vivo MRI experiments were performed to separately test cell transplantation and cell migration paradigms, as well as in vivo biodegradation.</p></div></div>
<div class="section" id="mrm24741-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Highly magnetic nano (∼100 nm) and microparticles (∼1–2 µm) were fabricated. Magnetic cell labeling in culture occurred rapidly achieving 3–50 pg Fe/cell at 3 h for different particles types, and &gt;100 pg Fe/cell after 10 h, without the requirement of a transfection agent, and with no effect on cell viability. The capability of magnetically labeled mesenchymal or neural stem cells to differentiate down multiple lineages, or for magnetically labeled immune cells to release cytokines following stimulation, was uncompromised. An in vivo biodegradation study revealed that NPs degraded ∼80% over the course of 12 weeks. MRI detected as few as 10 magnetically labeled cells, transplanted into the brains of rats. Also, these particles enabled the in vivo monitoring of endogenous neural progenitor cell migration in rat brains over 2 weeks.</p></div></div>
<div class="section" id="mrm24741-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The robust MRI properties and benign safety profile of these particles make them promising candidates for clinical translation for MRI-based cell tracking. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
To design, fabricate, characterize, and in vivo assay clinically viable magnetic particles for MRI-based cell tracking.


Methods
Poly(lactide-co-glycolide) (PLGA) encapsulated magnetic nano and microparticles were fabricated. Multiple biologically relevant experiments were performed to assess cell viability, cellular performance, and stem cell differentiation. In vivo MRI experiments were performed to separately test cell transplantation and cell migration paradigms, as well as in vivo biodegradation.


Results
Highly magnetic nano (∼100 nm) and microparticles (∼1–2 µm) were fabricated. Magnetic cell labeling in culture occurred rapidly achieving 3–50 pg Fe/cell at 3 h for different particles types, and &gt;100 pg Fe/cell after 10 h, without the requirement of a transfection agent, and with no effect on cell viability. The capability of magnetically labeled mesenchymal or neural stem cells to differentiate down multiple lineages, or for magnetically labeled immune cells to release cytokines following stimulation, was uncompromised. An in vivo biodegradation study revealed that NPs degraded ∼80% over the course of 12 weeks. MRI detected as few as 10 magnetically labeled cells, transplanted into the brains of rats. Also, these particles enabled the in vivo monitoring of endogenous neural progenitor cell migration in rat brains over 2 weeks.


Conclusion
The robust MRI properties and benign safety profile of these particles make them promising candidates for clinical translation for MRI-based cell tracking. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24740" xmlns="http://purl.org/rss/1.0/"><title>High-resolution mouse kidney perfusion imaging by pseudo-continuous arterial spin labeling at 11.75T</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24740</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High-resolution mouse kidney perfusion imaging by pseudo-continuous arterial spin labeling at 11.75T</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Guillaume Duhamel, Valentin Prevost, Olivier M. Girard, Virginie Callot, Patrick J. Cozzone</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T08:11:01.477674-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24740</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24740</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24740</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24740-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Quantitative measure of blood flow provides important information regarding renal function, nephropathies and viability of kidney transplantation. Therefore, a method that would allow quantitative and reliable assessment of the renal microvascular perfusion would be very valuable. Arterial spin labeling Magnetic Resonance Imaging has started to be widely used for human studies. For rodents though, despite the increasing number of transgenic mouse models, renal perfusion Magnetic Resonance Imaging has been only sparsely reported. This study investigated the use of FAIR (flow-sensitive alternating inversion recovery) and pseudo-continuous arterial spin labeling (pCASL) for mouse renal blood flow measurements.</p></div></div>
<div class="section" id="mrm24740-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>FAIR and pCASL were compared in terms of sensitivity, absolute quantification, reproducibility and flexibility of implementation. Multislice and coronal imaging were also investigated. Studies were performed at 11.75 T with volumic transmitter/receiver radiofrequency coils and fast imaging.</p></div></div>
<div class="section" id="mrm24740-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>pCASL demonstrated better experimental flexibility and higher sensitivity compared to FAIR (&gt; +20%). Renal blood flow values in the range of 550–750 mL/100 g/min for the cortex and of 140–230 mL/100 g/min for the medulla, consistent with literature data, were measured.</p></div></div>
<div class="section" id="mrm24740-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>pCASL was successfully applied at very high field for mouse renal blood flow measurements, demonstrating high sensitivity, flexibility and multislice imaging capability. pCASL may be considered as a method of choice for mouse kidney perfusion studies. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Quantitative measure of blood flow provides important information regarding renal function, nephropathies and viability of kidney transplantation. Therefore, a method that would allow quantitative and reliable assessment of the renal microvascular perfusion would be very valuable. Arterial spin labeling Magnetic Resonance Imaging has started to be widely used for human studies. For rodents though, despite the increasing number of transgenic mouse models, renal perfusion Magnetic Resonance Imaging has been only sparsely reported. This study investigated the use of FAIR (flow-sensitive alternating inversion recovery) and pseudo-continuous arterial spin labeling (pCASL) for mouse renal blood flow measurements.


Methods
FAIR and pCASL were compared in terms of sensitivity, absolute quantification, reproducibility and flexibility of implementation. Multislice and coronal imaging were also investigated. Studies were performed at 11.75 T with volumic transmitter/receiver radiofrequency coils and fast imaging.


Results
pCASL demonstrated better experimental flexibility and higher sensitivity compared to FAIR (&gt; +20%). Renal blood flow values in the range of 550–750 mL/100 g/min for the cortex and of 140–230 mL/100 g/min for the medulla, consistent with literature data, were measured.


Conclusion
pCASL was successfully applied at very high field for mouse renal blood flow measurements, demonstrating high sensitivity, flexibility and multislice imaging capability. pCASL may be considered as a method of choice for mouse kidney perfusion studies. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24735" xmlns="http://purl.org/rss/1.0/"><title>Cardiac functional assessment without electrocardiogram using physiological self-navigation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24735</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cardiac functional assessment without electrocardiogram using physiological self-navigation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Christoph Kolbitsch, Claudia Prieto, Tobias Schaeffter</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-08T08:10:54.129349-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24735</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24735</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24735</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24735-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Electrocardiogram (ECG)-gated cine MRI provides highly accurate functional assessment of the heart. Nevertheless, reliable ECG signals are not always available due to patient's electrophysiology or due to high MR field strengths. Here, a novel framework for cardiac functional assessment using physiological information is presented, which is obtained from MR image data.</p></div></div>
<div class="section" id="mrm24735-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Multiple long-axis slices rotated around the center axis of the left ventricle are acquired using a 2D Golden Radial acquisition scheme. This sampling approach allows for both real-time data and retrospectively reordered cine images with different temporal resolutions. Functional information from the left ventricle is used for retrospective reordering of the data to reconstruct cine images without an external ECG signal. Afterward, individual 2D cine slices are synchronized using physiological information on the mitral valve closure. The proposed approach was assessed in 15 volunteers and applied in four patients for feasibility.</p></div></div>
<div class="section" id="mrm24735-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Physiological gating signals obtained with our approach show great correlation with an ECG reference signal. Functional parameters determined with the presented method show a relative difference of less than 1.3% when compared with an ECG-gated approach.</p></div></div>
<div class="section" id="mrm24735-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>It is successfully demonstrated that functional assessment of the heart is possible using physiological information obtained directly from MR image data. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Electrocardiogram (ECG)-gated cine MRI provides highly accurate functional assessment of the heart. Nevertheless, reliable ECG signals are not always available due to patient's electrophysiology or due to high MR field strengths. Here, a novel framework for cardiac functional assessment using physiological information is presented, which is obtained from MR image data.


Methods
Multiple long-axis slices rotated around the center axis of the left ventricle are acquired using a 2D Golden Radial acquisition scheme. This sampling approach allows for both real-time data and retrospectively reordered cine images with different temporal resolutions. Functional information from the left ventricle is used for retrospective reordering of the data to reconstruct cine images without an external ECG signal. Afterward, individual 2D cine slices are synchronized using physiological information on the mitral valve closure. The proposed approach was assessed in 15 volunteers and applied in four patients for feasibility.


Results
Physiological gating signals obtained with our approach show great correlation with an ECG reference signal. Functional parameters determined with the presented method show a relative difference of less than 1.3% when compared with an ECG-gated approach.


Conclusion
It is successfully demonstrated that functional assessment of the heart is possible using physiological information obtained directly from MR image data. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24734" xmlns="http://purl.org/rss/1.0/"><title>Reconstruction of magnetic resonance imaging by three-dimensional dual-dictionary learning</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24734</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Reconstruction of magnetic resonance imaging by three-dimensional dual-dictionary learning</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ying Song, Zhen Zhu, Yang Lu, Qiegen Liu, Jun Zhao</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-02T15:21:42.197311-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24734</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24734</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24734</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24734-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To improve the magnetic resonance imaging (MRI) data acquisition speed while maintaining the reconstruction quality, a novel method is proposed for multislice MRI reconstruction from undersampled k-space data based on compressed-sensing theory using dictionary learning.</p></div></div>
<div class="section" id="mrm24734-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>There are two aspects to improve the reconstruction quality. One is that spatial correlation among slices is used by extending the atoms in dictionary learning from patches to blocks. The other is that the dictionary-learning scheme is used at two resolution levels; i.e., a low-resolution dictionary is used for sparse coding and a high-resolution dictionary is used for image updating. Numerical experiments are carried out on in vivo 3D MR images of brains and abdomens with a variety of undersampling schemes and ratios.</p></div></div>
<div class="section" id="mrm24734-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The proposed method (dual-DLMRI) achieves better reconstruction quality than conventional reconstruction methods, with the peak signal-to-noise ratio being 7 dB higher. The advantages of the dual dictionaries are obvious compared with the single dictionary. Parameter variations ranging from 50% to 200% only bias the image quality within 15% in terms of the peak signal-to-noise ratio.</p></div></div>
<div class="section" id="mrm24734-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Dual-DLMRI effectively uses the a priori information in the dual-dictionary scheme and provides dramatically improved reconstruction quality.</p></div></div>
]]></content:encoded><description>

Purpose
To improve the magnetic resonance imaging (MRI) data acquisition speed while maintaining the reconstruction quality, a novel method is proposed for multislice MRI reconstruction from undersampled k-space data based on compressed-sensing theory using dictionary learning.


Theory and Methods
There are two aspects to improve the reconstruction quality. One is that spatial correlation among slices is used by extending the atoms in dictionary learning from patches to blocks. The other is that the dictionary-learning scheme is used at two resolution levels; i.e., a low-resolution dictionary is used for sparse coding and a high-resolution dictionary is used for image updating. Numerical experiments are carried out on in vivo 3D MR images of brains and abdomens with a variety of undersampling schemes and ratios.


Results
The proposed method (dual-DLMRI) achieves better reconstruction quality than conventional reconstruction methods, with the peak signal-to-noise ratio being 7 dB higher. The advantages of the dual dictionaries are obvious compared with the single dictionary. Parameter variations ranging from 50% to 200% only bias the image quality within 15% in terms of the peak signal-to-noise ratio.


Conclusion
Dual-DLMRI effectively uses the a priori information in the dual-dictionary scheme and provides dramatically improved reconstruction quality.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24738" xmlns="http://purl.org/rss/1.0/"><title>Auto-calibration approach for k–t SENSE</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24738</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Auto-calibration approach for k–t SENSE</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Irene P. Ponce, Martin Blaimer, Felix A. Breuer, Mark A. Griswold, Peter M. Jakob, Peter Kellman</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-02T15:17:33.588384-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24738</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24738</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24738</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24738-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The goal of this work is to increase the spatial resolution of training data, used by reconstruction methods such as k–t SENSE in order to calculate the missing data in a series of dynamic images, without compromising their temporal resolution or acquisition time.</p></div></div>
<div class="section" id="mrm24738-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory</h4><div class="para"><p>The k-t SENSE method allows dynamic imaging at high acceleration factors with high reconstruction quality. However, the low resolution training data required by k-t SENSE may cause undesired temporal filtering effects in the reconstructed images.</p></div></div>
<div class="section" id="mrm24738-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>In this work, a feedback regularization approach is applied to realize auto-calibration of the k-t SENSE algorithm. To that end, a full resolution training data set is calculated from the accelerated data itself using a TSENSE reconstruction. The reconstructed training data are then fed back for the actual k-t SENSE reconstruction. For evaluation of our approach, temporal filtering effects are quantified by calculating the modulation transfer function and noise measurements are done by Monte-Carlo simulations.</p></div></div>
<div class="section" id="mrm24738-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Computer simulations and cardiac imaging experiments demonstrate an improved temporal fidelity of auto-calibrated k-t SENSE compared to standard k-t SENSE.</p></div></div>
<div class="section" id="mrm24738-sec-0005" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Auto-calibrated k-t SENSE provides high quality reconstructions for dynamic imaging applications. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The goal of this work is to increase the spatial resolution of training data, used by reconstruction methods such as k–t SENSE in order to calculate the missing data in a series of dynamic images, without compromising their temporal resolution or acquisition time.


Theory
The k-t SENSE method allows dynamic imaging at high acceleration factors with high reconstruction quality. However, the low resolution training data required by k-t SENSE may cause undesired temporal filtering effects in the reconstructed images.


Methods
In this work, a feedback regularization approach is applied to realize auto-calibration of the k-t SENSE algorithm. To that end, a full resolution training data set is calculated from the accelerated data itself using a TSENSE reconstruction. The reconstructed training data are then fed back for the actual k-t SENSE reconstruction. For evaluation of our approach, temporal filtering effects are quantified by calculating the modulation transfer function and noise measurements are done by Monte-Carlo simulations.


Results
Computer simulations and cardiac imaging experiments demonstrate an improved temporal fidelity of auto-calibrated k-t SENSE compared to standard k-t SENSE.


Conclusion
Auto-calibrated k-t SENSE provides high quality reconstructions for dynamic imaging applications. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24729" xmlns="http://purl.org/rss/1.0/"><title>Probing lung microstructure with hyperpolarized noble gas diffusion MRI: theoretical models and experimental results</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24729</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Probing lung microstructure with hyperpolarized noble gas diffusion MRI: theoretical models and experimental results</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dmitriy A. Yablonskiy, Alexander L. Sukstanskii, James D. Quirk, Jason C. Woods, Mark S. Conradi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-02T15:16:30.257199-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24729</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24729</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24729</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Review Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The introduction of hyperpolarized gases (<sup>3</sup>He and <sup>129</sup>Xe) has opened the door to applications for which gaseous agents are uniquely suited—lung MRI. One of the pulmonary applications, diffusion MRI, relies on measuring Brownian motion of inhaled hyperpolarized gas atoms diffusing in lung airspaces. In this article we provide an overview of the theoretical ideas behind hyperpolarized gas diffusion MRI and the results obtained over the decade-long research. We describe a simple technique based on measuring gas apparent diffusion coefficient (ADC) and an advanced technique, in vivo lung morphometry, that quantifies lung microstructure both in terms of Weibel parameters (acinar airways radii and alveolar depth) and standard metrics (mean linear intercept, surface-to-volume ratio, and alveolar density) that are widely used by lung researchers but were previously available only from invasive lung biopsy. This technique has the ability to provide unique three-dimensional tomographic information on lung microstructure from a less than 15 s MRI scan with results that are in good agreement with direct histological measurements. These safe and sensitive diffusion measurements improve our understanding of lung structure and functioning in health and disease, providing a platform for monitoring the efficacy of therapeutic interventions in clinical trials. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div>
]]></content:encoded><description>
The introduction of hyperpolarized gases (3He and 129Xe) has opened the door to applications for which gaseous agents are uniquely suited—lung MRI. One of the pulmonary applications, diffusion MRI, relies on measuring Brownian motion of inhaled hyperpolarized gas atoms diffusing in lung airspaces. In this article we provide an overview of the theoretical ideas behind hyperpolarized gas diffusion MRI and the results obtained over the decade-long research. We describe a simple technique based on measuring gas apparent diffusion coefficient (ADC) and an advanced technique, in vivo lung morphometry, that quantifies lung microstructure both in terms of Weibel parameters (acinar airways radii and alveolar depth) and standard metrics (mean linear intercept, surface-to-volume ratio, and alveolar density) that are widely used by lung researchers but were previously available only from invasive lung biopsy. This technique has the ability to provide unique three-dimensional tomographic information on lung microstructure from a less than 15 s MRI scan with results that are in good agreement with direct histological measurements. These safe and sensitive diffusion measurements improve our understanding of lung structure and functioning in health and disease, providing a platform for monitoring the efficacy of therapeutic interventions in clinical trials. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24733" xmlns="http://purl.org/rss/1.0/"><title>Storage of magnetization as singlet order by optimal control designed pulses</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24733</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Storage of magnetization as singlet order by optimal control designed pulses</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Christoffer Laustsen, Sean Bowen, Mads Sloth Vinding, Niels Chr. Nielsen, Jan H. Ardenkjaer-Larsen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-02T15:04:48.252384-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24733</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24733</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24733</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24733-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The use of hyperpolarization to enhance the sensitivity of MRI has so far been limited by the decay of the polarization through <em>T</em><sub>1</sub> relaxation. Recently, methods have been proposed that extend the lifetime of the hyperpolarization by storing the spin order in slowly relaxing singlet states.</p></div></div>
<div class="section" id="mrm24733-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>With this aim, optimal control theory was applied to create pulses that for near-equivalent spins accomplish transfers in and out of the singlet state with maximum efficiency while ensuring robustness toward variations in the nuclear spin system Hamiltonian (chemical shift, <em>J</em>-couplings, <em>B</em><sub>1</sub> and <em>B</em><sub>0</sub> magnetic field inhomogeneity).</p></div></div>
<div class="section" id="mrm24733-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The pulses are designed to accomplish efficient transfer with low <em>B</em><sub>1</sub> amplitude, essential for applications on preclinical and clinical MR scanners.</p></div></div>
<div class="section" id="mrm24733-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>It is demonstrated that significantly improved efficiency and robustness can be obtained within the limitations of typical MR scanner performance.</p></div></div>
]]></content:encoded><description>

Purpose
The use of hyperpolarization to enhance the sensitivity of MRI has so far been limited by the decay of the polarization through T1 relaxation. Recently, methods have been proposed that extend the lifetime of the hyperpolarization by storing the spin order in slowly relaxing singlet states.


Methods
With this aim, optimal control theory was applied to create pulses that for near-equivalent spins accomplish transfers in and out of the singlet state with maximum efficiency while ensuring robustness toward variations in the nuclear spin system Hamiltonian (chemical shift, J-couplings, B1 and B0 magnetic field inhomogeneity).


Results
The pulses are designed to accomplish efficient transfer with low B1 amplitude, essential for applications on preclinical and clinical MR scanners.


Conclusion
It is demonstrated that significantly improved efficiency and robustness can be obtained within the limitations of typical MR scanner performance.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24659" xmlns="http://purl.org/rss/1.0/"><title>Triple echo steady-state (TESS) relaxometry</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24659</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Triple echo steady-state (TESS) relaxometry</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rahel Heule, Carl Ganter, Oliver Bieri</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-02T15:03:10.498114-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24659</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24659</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24659</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24659-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Rapid imaging techniques have attracted increased interest for relaxometry, but none are perfect: they are prone to static (<em>B</em><sub>0</sub>) and transmit (<em>B</em><sub>1</sub>) field heterogeneities, and commonly biased by <em>T</em><sub>2</sub>/<em>T</em><sub>1</sub>. The purpose of this study is the development of a rapid <em>T</em><sub>1</sub> and <em>T</em><sub>2</sub> relaxometry method that is completely (<em>T</em><sub>2</sub>) or partly (<em>T</em><sub>1</sub>) bias-free.</p></div></div>
<div class="section" id="mrm24659-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A new method is introduced to simultaneously quantify <em>T</em><sub>1</sub> and <em>T</em><sub>2</sub> within one single scan based on a triple echo steady-state (TESS) approach in combination with an iterative golden section search. TESS relaxometry is optimized and evaluated from simulations, in vitro studies, and in vivo experiments.</p></div></div>
<div class="section" id="mrm24659-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>It is found that relaxometry with TESS is not biased by <em>T</em><sub>2</sub>/<em>T</em><sub>1</sub>, insensitive to <em>B</em><sub>0</sub> heterogeneities, and, surprisingly, that TESS-<em>T</em><sub>2</sub> is not affected by <em>B</em><sub>1</sub> field errors. Consequently, excellent correspondence between TESS and reference spin echo data is observed for <em>T</em><sub>2</sub> in vitro at 1.5 T and in vivo at 3 T.</p></div></div>
<div class="section" id="mrm24659-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>TESS offers rapid <em>T</em><sub>1</sub> and <em>T</em><sub>2</sub> quantification within one single scan, and in particular <em>B</em><sub>1</sub>-insensitive <em>T</em><sub>2</sub> estimation. As a result, the new proposed method is of high interest for fast and reliable high-resolution <em>T</em><sub>2</sub> mapping, especially of the musculoskeletal system at high to ultra-high fields. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Rapid imaging techniques have attracted increased interest for relaxometry, but none are perfect: they are prone to static (B0) and transmit (B1) field heterogeneities, and commonly biased by T2/T1. The purpose of this study is the development of a rapid T1 and T2 relaxometry method that is completely (T2) or partly (T1) bias-free.


Methods
A new method is introduced to simultaneously quantify T1 and T2 within one single scan based on a triple echo steady-state (TESS) approach in combination with an iterative golden section search. TESS relaxometry is optimized and evaluated from simulations, in vitro studies, and in vivo experiments.


Results
It is found that relaxometry with TESS is not biased by T2/T1, insensitive to B0 heterogeneities, and, surprisingly, that TESS-T2 is not affected by B1 field errors. Consequently, excellent correspondence between TESS and reference spin echo data is observed for T2 in vitro at 1.5 T and in vivo at 3 T.


Conclusion
TESS offers rapid T1 and T2 quantification within one single scan, and in particular B1-insensitive T2 estimation. As a result, the new proposed method is of high interest for fast and reliable high-resolution T2 mapping, especially of the musculoskeletal system at high to ultra-high fields. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24737" xmlns="http://purl.org/rss/1.0/"><title>Phase-labeled reference EPI for frequency-segmented inhomogeneity corrections (PREFICS)</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24737</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Phase-labeled reference EPI for frequency-segmented inhomogeneity corrections (PREFICS)</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mario Zeller, Alexander Müller, Dietbert Hahn, Herbert Köstler</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-29T08:05:42.337344-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24737</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24737</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24737</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24737-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To develop a method to correct for geometric distortions in non-Cartesian echo planar imaging using data acquired in a fast prescan.</p></div></div>
<div class="section" id="mrm24737-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Echo planar images were obtained using a non-Cartesian density weighted k-space trajectory. In contrast to linear Cartesian acquisition, distortions arising in non-Cartesian acquisitions can only be corrected using conjugate phase-based methods. Up to now these methods require a time consuming field map acquisition in undistorted coordinates. In this work, a phase-labeled reference EPI scan was performed in a very short time, yielding a displacement map in distorted coordinates. Subsequently, this map was applied to itself and thus transformed into undistorted coordinates. The echo planar images were then corrected with a frequency-segmented conjugate phase method. The results were compared with corrections based on a multi-echo reference field map acquired in undistorted coordinates.</p></div></div>
<div class="section" id="mrm24737-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Uncorrected density weighted EPI exhibited geometric distortions and severe ringing artifacts. These distortions could be successfully corrected using the novel method. The quality was comparable to corrections based on the multi-echo reference field map. The novel method shortens the field map acquisition duration by a factor of 64.</p></div></div>
<div class="section" id="mrm24737-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The method presented allows correcting non-Cartesian EPI from a reference scan consisting of only two phase-labeled echo planar images. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To develop a method to correct for geometric distortions in non-Cartesian echo planar imaging using data acquired in a fast prescan.


Methods
Echo planar images were obtained using a non-Cartesian density weighted k-space trajectory. In contrast to linear Cartesian acquisition, distortions arising in non-Cartesian acquisitions can only be corrected using conjugate phase-based methods. Up to now these methods require a time consuming field map acquisition in undistorted coordinates. In this work, a phase-labeled reference EPI scan was performed in a very short time, yielding a displacement map in distorted coordinates. Subsequently, this map was applied to itself and thus transformed into undistorted coordinates. The echo planar images were then corrected with a frequency-segmented conjugate phase method. The results were compared with corrections based on a multi-echo reference field map acquired in undistorted coordinates.


Results
Uncorrected density weighted EPI exhibited geometric distortions and severe ringing artifacts. These distortions could be successfully corrected using the novel method. The quality was comparable to corrections based on the multi-echo reference field map. The novel method shortens the field map acquisition duration by a factor of 64.


Conclusion
The method presented allows correcting non-Cartesian EPI from a reference scan consisting of only two phase-labeled echo planar images. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24725" xmlns="http://purl.org/rss/1.0/"><title>Noninvasive assessment of osteoarthritis severity in human explants by multicontrast MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24725</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Noninvasive assessment of osteoarthritis severity in human explants by multicontrast MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Adam J. Griebel, Stephen B. Trippel, Nancy C. Emery, Corey P. Neu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-29T07:52:04.277854-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24725</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24725</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24725</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24725-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Medical imaging has the potential to noninvasively diagnose early disease onset and monitor the success of repair therapies. Unfortunately, few reliable imaging biomarkers exist to detect cartilage diseases before advanced degeneration in the tissue.</p></div></div>
<div class="section" id="mrm24725-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Method</h4><div class="para"><p>In this study, we quantified the ability to detect osteoarthritis (OA) severity in human cartilage explants using a multicontrast magnetic resonance imaging (MRI) approach, inclusive of novel displacements under applied loading by MRI, relaxivity measures, and standard MRI.</p></div></div>
<div class="section" id="mrm24725-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Displacements under applied loading by MRI measures, which characterized the spatial micromechanical environment by 2D finite and Von Mises strains, were strong predictors of histologically assessed OA severity, both before and after controlling for factors, e.g., patient, joint region, and morphology. Relaxivity measures, sensitive to local macromolecular weight and composition, including <em>T</em><sub>1ρ</sub>, but not <em>T</em><sub>1</sub> or <em>T</em><sub>2</sub>, were predictors of OA severity. A combined multicontrast approach that exploited spatial variations in tissue biomechanics and extracellular matrix structure yielded the strongest relationships to OA severity.</p></div></div>
<div class="section" id="mrm24725-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Our results indicate that combining multiple MRI-based biomarkers has high potential for the noninvasive measurement of OA severity and the evaluation of potential therapeutic agents used in the treatment of early OA in animal and human trials. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Medical imaging has the potential to noninvasively diagnose early disease onset and monitor the success of repair therapies. Unfortunately, few reliable imaging biomarkers exist to detect cartilage diseases before advanced degeneration in the tissue.


Method
In this study, we quantified the ability to detect osteoarthritis (OA) severity in human cartilage explants using a multicontrast magnetic resonance imaging (MRI) approach, inclusive of novel displacements under applied loading by MRI, relaxivity measures, and standard MRI.


Results
Displacements under applied loading by MRI measures, which characterized the spatial micromechanical environment by 2D finite and Von Mises strains, were strong predictors of histologically assessed OA severity, both before and after controlling for factors, e.g., patient, joint region, and morphology. Relaxivity measures, sensitive to local macromolecular weight and composition, including T1ρ, but not T1 or T2, were predictors of OA severity. A combined multicontrast approach that exploited spatial variations in tissue biomechanics and extracellular matrix structure yielded the strongest relationships to OA severity.


Conclusion
Our results indicate that combining multiple MRI-based biomarkers has high potential for the noninvasive measurement of OA severity and the evaluation of potential therapeutic agents used in the treatment of early OA in animal and human trials. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24702" xmlns="http://purl.org/rss/1.0/"><title>Four-channel surface coil array for 300-MHz pulsed EPR imaging: Proof-of-concept experiments</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24702</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Four-channel surface coil array for 300-MHz pulsed EPR imaging: Proof-of-concept experiments</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ayano Enomoto, Hiroshi Hirata, Shingo Matsumoto, Keita Saito, Sankaran Subramanian, Murali C. Krishna, Nallathamby Devasahayam</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-26T07:48:12.569158-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24702</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24702</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24702</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Time-domain electron paramagnetic resonance imaging is currently a useful preclinical molecular imaging modality in experimental animals such as mice and is capable of quantitatively mapping hypoxia in tumor implants. The microseconds range relaxation times (<em>T</em><sub>1</sub> and <em>T</em><sub>2</sub>) of paramagnetic tracers and the large bandwidths (tens of MHz) to be excited by electron paramagnetic resonance pulses for spatial encoding makes imaging of large objects a challenging task. The possibility of using multiple array coils to permit studies on large sized object is the purpose of the present work. Toward this end, the use of planar array coils in different configurations to image larger objects than cannot be fully covered by a single resonator element is explored. Multiple circular surface coils, which are arranged in a plane or at suitable angles mimicking a volume resonator, are used in imaging a phantom and a tumor-bearing mouse leg. The image was formed by combining the images collected from the individual coils with suitable scaling. The results support such a possibility. By multiplexing or interleaving the measurements from each element of such array resonators, one can scale up the size of the subject and at the same time reduce the radiofrequency power requirements and increase the sensitivity. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div>
]]></content:encoded><description>
Time-domain electron paramagnetic resonance imaging is currently a useful preclinical molecular imaging modality in experimental animals such as mice and is capable of quantitatively mapping hypoxia in tumor implants. The microseconds range relaxation times (T1 and T2) of paramagnetic tracers and the large bandwidths (tens of MHz) to be excited by electron paramagnetic resonance pulses for spatial encoding makes imaging of large objects a challenging task. The possibility of using multiple array coils to permit studies on large sized object is the purpose of the present work. Toward this end, the use of planar array coils in different configurations to image larger objects than cannot be fully covered by a single resonator element is explored. Multiple circular surface coils, which are arranged in a plane or at suitable angles mimicking a volume resonator, are used in imaging a phantom and a tumor-bearing mouse leg. The image was formed by combining the images collected from the individual coils with suitable scaling. The results support such a possibility. By multiplexing or interleaving the measurements from each element of such array resonators, one can scale up the size of the subject and at the same time reduce the radiofrequency power requirements and increase the sensitivity. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24664" xmlns="http://purl.org/rss/1.0/"><title>In vivo maps of extracellular pH in murine melanoma by CEST–MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24664</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">In vivo maps of extracellular pH in murine melanoma by CEST–MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Delli Castelli D, Giuseppe Ferrauto, Juan Carlos Cutrin, Enzo Terreno, Silvio Aime</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-25T11:15:52.661647-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24664</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24664</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24664</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24664-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>A novel method based on the use of Yb-HPDO3A as MRI Para-CEST agent for in vivo pH mapping of the tumor region in a melanoma murine model is reported. This method does not require the knowledge of the concentration of the imaging agent.</p></div></div>
<div class="section" id="mrm24664-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>C57BL/6-mice were inoculated with B16-F10 cells. CEST–MR images of tumor and bladder were acquired upon the i.v. administration of Yb-HPDO3A (1.2 mmol/Kg). pH was assessed by the use of a ratiometric method.</p></div></div>
<div class="section" id="mrm24664-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Yb-HPDO3A distributes well in the extracellular space of the tumor allowing the detection of good levels of saturation transfer (ST). It is excreted throughout kidneys and accumulated in the bladder thus yielding a strong CEST signal from urine. By comparing the ST% obtained upon selective irradiation of the two <img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>OH resonances belonging to the two isomeric forms of Yb-HPDO3A, it has been possible to measure the extracellular pH for each voxel (0.22 mm<sup>3</sup>). The obtained pH-maps of tumors show a great heterogeneity. Marked differences are associated to tumor staging.</p></div></div>
<div class="section" id="mrm24664-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The application of Yb-HPDO3A to measure extracellular tumor pH provides a good spatio-temporal resolution and it does not require the prior knowledge of the contrast agent concentration. The herein reported data support the potential clinical translation of Yb-HPDO3A. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
A novel method based on the use of Yb-HPDO3A as MRI Para-CEST agent for in vivo pH mapping of the tumor region in a melanoma murine model is reported. This method does not require the knowledge of the concentration of the imaging agent.


Methods
C57BL/6-mice were inoculated with B16-F10 cells. CEST–MR images of tumor and bladder were acquired upon the i.v. administration of Yb-HPDO3A (1.2 mmol/Kg). pH was assessed by the use of a ratiometric method.


Results
Yb-HPDO3A distributes well in the extracellular space of the tumor allowing the detection of good levels of saturation transfer (ST). It is excreted throughout kidneys and accumulated in the bladder thus yielding a strong CEST signal from urine. By comparing the ST% obtained upon selective irradiation of the two <img src="http://onlinelibrarystatic.wiley.com/undisplayable_characters/00f8ff.gif" alt="[BOND]"/>OH resonances belonging to the two isomeric forms of Yb-HPDO3A, it has been possible to measure the extracellular pH for each voxel (0.22 mm3). The obtained pH-maps of tumors show a great heterogeneity. Marked differences are associated to tumor staging.


Conclusion
The application of Yb-HPDO3A to measure extracellular tumor pH provides a good spatio-temporal resolution and it does not require the prior knowledge of the contrast agent concentration. The herein reported data support the potential clinical translation of Yb-HPDO3A. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24727" xmlns="http://purl.org/rss/1.0/"><title>High-spatial and high-temporal resolution dynamic contrast-enhanced perfusion imaging of the liver with time-resolved three-dimensional radial MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24727</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High-spatial and high-temporal resolution dynamic contrast-enhanced perfusion imaging of the liver with time-resolved three-dimensional radial MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ethan K. Brodsky, Eric M. Bultman, Kevin M. Johnson, Debra E. Horng, William R. Schelman, Walter F. Block, Scott B. Reeder</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-20T08:26:46.423577-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24727</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24727</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24727</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24727-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Detection, characterization, and monitoring the treatment of hepatocellular carcinomas (HCC) in patients with cirrhosis is challenging because of their variable and rapid arterial enhancement. Multiphase dynamic contrast-enhanced MRI is used clinically for HCC assessment; however, the method suffers from limited temporal resolution and difficulty in coordinating imaging and breath-hold timing within a narrow temporal window of interest. In this article, a volumetric, high-spatial resolution, and high-temporal resolution dynamic contrast-enhanced liver imaging method for improved detection and characterization of HCC is demonstrated.</p></div></div>
<div class="section" id="mrm24727-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A time-resolved three-dimensional radial acquisition with iterative sensitivity-encoding reconstruction images the entire abdomen and thorax with high spatial and temporal resolution, using real-time three-dimensional fluoroscopy to match the breath hold to contrast arrival. The sequence was tested on 17 subjects, including eight patients with HCC or other hypervascular focal lesions.</p></div></div>
<div class="section" id="mrm24727-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>This technique was successful in acquiring volumetric imaging of the entire liver with 2.1-mm isotropic spatial and true 4-s temporal resolution.</p></div></div>
<div class="section" id="mrm24727-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>This technique may be suitable for detecting, characterizing, and monitoring the treatment of HCC. It also holds significant potential for perfusion modeling, which may provide a noninvasive means to rapidly determine the efficacy of chemotherapeutic agents in these tumors over the entire liver volume. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Detection, characterization, and monitoring the treatment of hepatocellular carcinomas (HCC) in patients with cirrhosis is challenging because of their variable and rapid arterial enhancement. Multiphase dynamic contrast-enhanced MRI is used clinically for HCC assessment; however, the method suffers from limited temporal resolution and difficulty in coordinating imaging and breath-hold timing within a narrow temporal window of interest. In this article, a volumetric, high-spatial resolution, and high-temporal resolution dynamic contrast-enhanced liver imaging method for improved detection and characterization of HCC is demonstrated.


Methods
A time-resolved three-dimensional radial acquisition with iterative sensitivity-encoding reconstruction images the entire abdomen and thorax with high spatial and temporal resolution, using real-time three-dimensional fluoroscopy to match the breath hold to contrast arrival. The sequence was tested on 17 subjects, including eight patients with HCC or other hypervascular focal lesions.


Results
This technique was successful in acquiring volumetric imaging of the entire liver with 2.1-mm isotropic spatial and true 4-s temporal resolution.


Conclusion
This technique may be suitable for detecting, characterizing, and monitoring the treatment of HCC. It also holds significant potential for perfusion modeling, which may provide a noninvasive means to rapidly determine the efficacy of chemotherapeutic agents in these tumors over the entire liver volume. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24716" xmlns="http://purl.org/rss/1.0/"><title>Sparse BLIP: BLind Iterative Parallel imaging reconstruction using compressed sensing</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24716</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Sparse BLIP: BLind Iterative Parallel imaging reconstruction using compressed sensing</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Huajun She, Rong-Rong Chen, Dong Liang, Edward V. R. DiBella, Leslie Ying</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T07:41:23.598417-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24716</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24716</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24716</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24716-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To develop a sensitivity-based parallel imaging reconstruction method to reconstruct iteratively both the coil sensitivities and MR image simultaneously based on their prior information.</p></div></div>
<div class="section" id="mrm24716-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Parallel magnetic resonance imaging reconstruction problem can be formulated as a multichannel sampling problem where solutions are sought analytically. However, the channel functions given by the coil sensitivities in parallel imaging are not known exactly and the estimation error usually leads to artifacts. In this study, we propose a new reconstruction algorithm, termed Sparse BLind Iterative Parallel, for blind iterative parallel imaging reconstruction using compressed sensing. The proposed algorithm reconstructs both the sensitivity functions and the image simultaneously from undersampled data. It enforces the sparseness constraint in the image as done in compressed sensing, but is different from compressed sensing in that the sensing matrix is unknown and additional constraint is enforced on the sensitivities as well. Both phantom and <em>in vivo</em> imaging experiments were carried out with retrospective undersampling to evaluate the performance of the proposed method.</p></div></div>
<div class="section" id="mrm24716-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Experiments show improvement in Sparse BLind Iterative Parallel reconstruction when compared with Sparse SENSE, JSENSE, IRGN-TV, and L<sub>1</sub>-SPIRiT reconstructions with the same number of measurements.</p></div></div>
<div class="section" id="mrm24716-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The proposed Sparse BLind Iterative Parallel algorithm reduces the reconstruction errors when compared to the state-of-the-art parallel imaging methods. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To develop a sensitivity-based parallel imaging reconstruction method to reconstruct iteratively both the coil sensitivities and MR image simultaneously based on their prior information.


Methods
Parallel magnetic resonance imaging reconstruction problem can be formulated as a multichannel sampling problem where solutions are sought analytically. However, the channel functions given by the coil sensitivities in parallel imaging are not known exactly and the estimation error usually leads to artifacts. In this study, we propose a new reconstruction algorithm, termed Sparse BLind Iterative Parallel, for blind iterative parallel imaging reconstruction using compressed sensing. The proposed algorithm reconstructs both the sensitivity functions and the image simultaneously from undersampled data. It enforces the sparseness constraint in the image as done in compressed sensing, but is different from compressed sensing in that the sensing matrix is unknown and additional constraint is enforced on the sensitivities as well. Both phantom and in vivo imaging experiments were carried out with retrospective undersampling to evaluate the performance of the proposed method.


Results
Experiments show improvement in Sparse BLind Iterative Parallel reconstruction when compared with Sparse SENSE, JSENSE, IRGN-TV, and L1-SPIRiT reconstructions with the same number of measurements.


Conclusion
The proposed Sparse BLind Iterative Parallel algorithm reduces the reconstruction errors when compared to the state-of-the-art parallel imaging methods. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24730" xmlns="http://purl.org/rss/1.0/"><title>Fast, variable system delay correction for spiral MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24730</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Fast, variable system delay correction for spiral MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Payal S. Bhavsar, Nicholas R. Zwart, James G. Pipe</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T07:41:03.402879-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24730</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24730</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24730</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24730-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Time-varying system delays and eddy currents can substantially reduce the image quality of spiral images. A new method is proposed to estimate variable system delays for spiral-based trajectories.</p></div></div>
<div class="section" id="mrm24730-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>This approach requires a minor modification of a conventional stack-of-spirals sequence and analyzes data collected on three overlapping orthogonal cylinders.</p></div></div>
<div class="section" id="mrm24730-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Initial results are presented for acquired and synthesized phantom data and in vivo data.</p></div></div>
<div class="section" id="mrm24730-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The proposed method includes gradient coupling effects, requires no phantom measurements or specialized hardware, is robust to off-resonance effects, and estimates independent continuous delays for each gradient channel over the data-sampling period. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Time-varying system delays and eddy currents can substantially reduce the image quality of spiral images. A new method is proposed to estimate variable system delays for spiral-based trajectories.


Methods
This approach requires a minor modification of a conventional stack-of-spirals sequence and analyzes data collected on three overlapping orthogonal cylinders.


Results
Initial results are presented for acquired and synthesized phantom data and in vivo data.


Conclusion
The proposed method includes gradient coupling effects, requires no phantom measurements or specialized hardware, is robust to off-resonance effects, and estimates independent continuous delays for each gradient channel over the data-sampling period. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24706" xmlns="http://purl.org/rss/1.0/"><title>On random walks and entropy in diffusion-weighted magnetic resonance imaging studies of neural tissue</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24706</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">On random walks and entropy in diffusion-weighted magnetic resonance imaging studies of neural tissue</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Carson Ingo, Richard L. Magin, Luis Colon-Perez, William Triplett, Thomas H. Mareci</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-18T07:33:01.191056-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24706</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24706</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24706</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>In diffusion-weighted MRI studies of neural tissue, the classical model assumes the statistical mechanics of Brownian motion and predicts a monoexponential signal decay. However, there have been numerous reports of signal decays that are not monoexponential, particularly in the white matter.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory:</h4><div class="para"><p>We modeled diffusion in neural tissue from the perspective of the continuous time random walk. The characteristic diffusion decay is represented by the Mittag-Leffler function, which relaxes a priori assumptions about the governing statistics. We then used entropy as a measure of the anomalous features for the characteristic function.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>Diffusion-weighted MRI experiments were performed on a fixed rat brain using an imaging spectrometer at 17.6 T with <em>b</em>-values arrayed up to 25,000 s/mm<sup>2</sup>. Additionally, we examined the impact of varying either the gradient strength, <em>q</em>, or mixing time, Δ, on the observed diffusion dynamics.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>In white and gray matter regions, the Mittag-Leffler and entropy parameters demonstrated new information regarding subdiffusion and produced different image contrast from that of the classical diffusion coefficient. The choice of weighting on <em>q</em> and Δ produced different image contrast within the regions of interest.</p></div></div>
<div class="section" id="abs1-5" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>We propose these parameters have the potential as biomarkers for morphology in neural tissue. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
In diffusion-weighted MRI studies of neural tissue, the classical model assumes the statistical mechanics of Brownian motion and predicts a monoexponential signal decay. However, there have been numerous reports of signal decays that are not monoexponential, particularly in the white matter.


Theory:
We modeled diffusion in neural tissue from the perspective of the continuous time random walk. The characteristic diffusion decay is represented by the Mittag-Leffler function, which relaxes a priori assumptions about the governing statistics. We then used entropy as a measure of the anomalous features for the characteristic function.


Methods:
Diffusion-weighted MRI experiments were performed on a fixed rat brain using an imaging spectrometer at 17.6 T with b-values arrayed up to 25,000 s/mm2. Additionally, we examined the impact of varying either the gradient strength, q, or mixing time, Δ, on the observed diffusion dynamics.


Results:
In white and gray matter regions, the Mittag-Leffler and entropy parameters demonstrated new information regarding subdiffusion and produced different image contrast from that of the classical diffusion coefficient. The choice of weighting on q and Δ produced different image contrast within the regions of interest.


Conclusion:
We propose these parameters have the potential as biomarkers for morphology in neural tissue. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24633" xmlns="http://purl.org/rss/1.0/"><title>High-resolution 3D radial bSSFP with IDEAL</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24633</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High-resolution 3D radial bSSFP with IDEAL</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Catherine J. Moran, Ethan K. Brodsky, Leah Henze Bancroft, Scott B. Reeder, Huanzhou Yu, Richard Kijowski, Dorothee Engel, Walter F. Block</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-15T10:41:40.509999-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24633</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24633</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24633</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Radial trajectories facilitate high-resolution balanced steady state free precession (bSSFP) because the efficient gradients provide more time to extend the trajectory in k-space. A number of radial bSSFP methods that support fat–water separation have been developed; however, most of these methods require an environment with limited <em>B</em><sub>0</sub> inhomogeneity. In this work, high-resolution bSSFP with fat–water separation is achieved in more challenging <em>B</em><sub>0</sub> environments by combining a 3D radial trajectory with the IDEAL chemical species separation method. A method to maintain very high resolution within the timing constraints of bSSFP and IDEAL is described using a dual-pass pulse sequence. The sampling of a unique set of radial lines at each echo time is investigated as a means to circumvent the longer scan time that IDEAL incurs as a multiecho acquisition. The manifestation of undersampling artifacts in this trajectory and their effect on chemical species separation are investigated in comparison to the case in which each echo samples the same set of radial lines. This new bSSFP method achieves 0.63 mm isotropic resolution in a 5-min scan and is demonstrated in difficult in vivo imaging environments, including the breast and a knee with ACL reconstruction hardware at 1.5 T. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div>
]]></content:encoded><description>
Radial trajectories facilitate high-resolution balanced steady state free precession (bSSFP) because the efficient gradients provide more time to extend the trajectory in k-space. A number of radial bSSFP methods that support fat–water separation have been developed; however, most of these methods require an environment with limited B0 inhomogeneity. In this work, high-resolution bSSFP with fat–water separation is achieved in more challenging B0 environments by combining a 3D radial trajectory with the IDEAL chemical species separation method. A method to maintain very high resolution within the timing constraints of bSSFP and IDEAL is described using a dual-pass pulse sequence. The sampling of a unique set of radial lines at each echo time is investigated as a means to circumvent the longer scan time that IDEAL incurs as a multiecho acquisition. The manifestation of undersampling artifacts in this trajectory and their effect on chemical species separation are investigated in comparison to the case in which each echo samples the same set of radial lines. This new bSSFP method achieves 0.63 mm isotropic resolution in a 5-min scan and is demonstrated in difficult in vivo imaging environments, including the breast and a knee with ACL reconstruction hardware at 1.5 T. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24724" xmlns="http://purl.org/rss/1.0/"><title>A new approach to shimming: The dynamically controlled adaptive current network</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24724</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A new approach to shimming: The dynamically controlled adaptive current network</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Chad. T. Harris, William B. Handler, Blaine A. Chronik</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-15T09:16:46.338373-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24724</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24724</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24724</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24724-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Magnetic field homogeneity is important in all aspects of magnetic resonance imaging. A new approach to increase field homogeneity is presented that allows dynamic and adaptive control over the flow of current over a single surface using a network of actively controlled solid-state switches.</p></div></div>
<div class="section" id="mrm24724-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Computer simulations were completed demonstrating the potential of this approach. Wire patterns were produced using the boundary element method to remove magnetic field inhomogeneities over multiple regions of interest. Field maps and regions of interest histograms were compared with and without the shim present. A prototype was constructed confirming the feasibility of this approach within the magnetic resonance environment. Metal–oxide–semiconductor field-effect transistors were used. Two field maps were acquired with the prototype producing gradient and offset field profiles, respectively. The experimental field profiles were compared with simulation.</p></div></div>
<div class="section" id="mrm24724-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The wire patterns significantly increased field homogeneity over all regions of interest investigated. The field profiles produced by the prototype matched simulation. No imaging artifacts were produced.</p></div></div>
<div class="section" id="mrm24724-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>An approach to control the shape of a current distribution over a single surface has been described. This method has the potential to improve field homogeneity over any desired region of interest and is particularly well suited for dynamic applications. The method is feasible with current technology and construction techniques. <b>Magn Reson Med 000:000–000, 2013. © 2013 Wiley Periodicals, Inc</b>.</p></div></div>
]]></content:encoded><description>

Purpose
Magnetic field homogeneity is important in all aspects of magnetic resonance imaging. A new approach to increase field homogeneity is presented that allows dynamic and adaptive control over the flow of current over a single surface using a network of actively controlled solid-state switches.


Methods
Computer simulations were completed demonstrating the potential of this approach. Wire patterns were produced using the boundary element method to remove magnetic field inhomogeneities over multiple regions of interest. Field maps and regions of interest histograms were compared with and without the shim present. A prototype was constructed confirming the feasibility of this approach within the magnetic resonance environment. Metal–oxide–semiconductor field-effect transistors were used. Two field maps were acquired with the prototype producing gradient and offset field profiles, respectively. The experimental field profiles were compared with simulation.


Results
The wire patterns significantly increased field homogeneity over all regions of interest investigated. The field profiles produced by the prototype matched simulation. No imaging artifacts were produced.


Conclusions
An approach to control the shape of a current distribution over a single surface has been described. This method has the potential to improve field homogeneity over any desired region of interest and is particularly well suited for dynamic applications. The method is feasible with current technology and construction techniques. Magn Reson Med 000:000–000, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24710" xmlns="http://purl.org/rss/1.0/"><title>Highly accelerated dynamic contrast enhanced imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24710</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Highly accelerated dynamic contrast enhanced imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Robert Marc Lebel, Jesse Jones, Jean-Christophe Ferre, Meng Law, Krishna S. Nayak</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-15T08:59:17.592715-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24710</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24710</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24710</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24710-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Dynamic contrast-enhanced imaging provides unique physiological information, notably the endothelial permeability (<em>K</em><sup>trans</sup>), and may improve the diagnosis and management of multiple pathologies. Current acquisition methods provide limited spatial-temporal resolution and field-of-view, often preventing characterization of the entire pathology and precluding measurement of the arterial input function. We present a method for highly accelerated dynamic imaging and demonstrate its utility for dynamic contrast-enhanced modeling.</p></div></div>
<div class="section" id="mrm24710-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>We propose a novel Poisson ellipsoid sampling scheme and enforce multiple spatial and temporal <em>l</em><sub>1</sub>-norm constraints during image reconstruction. Retrospective and prospective analyses were performed to validate the approach.</p></div></div>
<div class="section" id="mrm24710-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Retrospectively, no mean bias or diverging trend was observed as the acceleration rate was increased from 3× to 18×; less than 10% error was measured in <em>K</em><sup>trans</sup> at any individual rates in this range. Prospectively accelerated images at a rate of 36× enabled full brain coverage with 0.94 × 0.94 × 1.9 mm<sup>3</sup> spatial and 4.1 s temporal resolutions. Images showed no visible degradation and provided accurate <em>K</em><sup>trans</sup> values when compared to a clinical population.</p></div></div>
<div class="section" id="mrm24710-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Highly accelerated dynamic MRI using compressed sensing and parallel imaging provides accurate permeability modeling and enables full brain, high resolution acquisitions. <b>Magn Reson Med 000:000–000, 2013. © 2013 Wiley Periodicals, Inc</b>.</p></div></div>
]]></content:encoded><description>

Purpose
Dynamic contrast-enhanced imaging provides unique physiological information, notably the endothelial permeability (Ktrans), and may improve the diagnosis and management of multiple pathologies. Current acquisition methods provide limited spatial-temporal resolution and field-of-view, often preventing characterization of the entire pathology and precluding measurement of the arterial input function. We present a method for highly accelerated dynamic imaging and demonstrate its utility for dynamic contrast-enhanced modeling.


Methods
We propose a novel Poisson ellipsoid sampling scheme and enforce multiple spatial and temporal l1-norm constraints during image reconstruction. Retrospective and prospective analyses were performed to validate the approach.


Results
Retrospectively, no mean bias or diverging trend was observed as the acceleration rate was increased from 3× to 18×; less than 10% error was measured in Ktrans at any individual rates in this range. Prospectively accelerated images at a rate of 36× enabled full brain coverage with 0.94 × 0.94 × 1.9 mm3 spatial and 4.1 s temporal resolutions. Images showed no visible degradation and provided accurate Ktrans values when compared to a clinical population.


Conclusion
Highly accelerated dynamic MRI using compressed sensing and parallel imaging provides accurate permeability modeling and enables full brain, high resolution acquisitions. Magn Reson Med 000:000–000, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24698" xmlns="http://purl.org/rss/1.0/"><title>Direct coronary motion extraction from a 2D fat image navigator for prospectively gated coronary MR angiography</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24698</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Direct coronary motion extraction from a 2D fat image navigator for prospectively gated coronary MR angiography</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Keigo Kawaji, Pascal Spincemaille, Thanh D. Nguyen, Nandadeepa Thimmappa, Mitchell A. Cooper, Martin R. Prince, Yi Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-15T08:59:09.176863-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24698</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24698</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24698</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24698-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Direct 2D tracking of cardiac motion may provide superior respiratory navigator gating for coronary magnetic resonance angiography compared to conventional liver-diaphragm navigators. However, additional 2D processing for motion extraction is unsuitable for real-time prospective gating. In this work, a 2D fat-selective image navigator, which delineates the epicardial fat surrounding coronary arteries, is developed to directly monitor epicardial fat motion at every heartbeat in real-time for prospective gating.</p></div></div>
<div class="section" id="mrm24698-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The proposed navigator is incorporated into a real-time interactive software that allows rapid setup and efficient motion extraction, and runs on standard clinical hardware without any additional dedicated components for processing. The proposed 2D cardiac fat image navigator was compared with the conventional 1D diaphragm navigator in free-breathing b-SSFP coronary MRAs in 12 healthy volunteers at 1.5T.</p></div></div>
<div class="section" id="mrm24698-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Real-time motion extraction from 2D cardiac fat navigator images was feasible within 20 ms, enabling successful prospectively gated coronary magnetic resonance angiographies in all subjects. Compared to 1D diaphragmatic navigator, 2D fat image navigator reduced scan time by 38% (<em>P</em> &lt; 0.0005), and significantly improved vessel sharpness, myocardial suppression, and image quality (<em>P</em> &lt; 0.05).</p></div></div>
<div class="section" id="mrm24698-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>This demonstrates the feasibility of a 3D SSFP coronary magnetic resonance angiography sequence using a 2D epicardial fat image as a navigator for real-time prospective motion tracking. <b>Magn Reson Med 000:000–000, 2013. © 2013 Wiley Periodicals, Inc</b>.</p></div></div>
]]></content:encoded><description>

Purpose
Direct 2D tracking of cardiac motion may provide superior respiratory navigator gating for coronary magnetic resonance angiography compared to conventional liver-diaphragm navigators. However, additional 2D processing for motion extraction is unsuitable for real-time prospective gating. In this work, a 2D fat-selective image navigator, which delineates the epicardial fat surrounding coronary arteries, is developed to directly monitor epicardial fat motion at every heartbeat in real-time for prospective gating.


Methods
The proposed navigator is incorporated into a real-time interactive software that allows rapid setup and efficient motion extraction, and runs on standard clinical hardware without any additional dedicated components for processing. The proposed 2D cardiac fat image navigator was compared with the conventional 1D diaphragm navigator in free-breathing b-SSFP coronary MRAs in 12 healthy volunteers at 1.5T.


Results
Real-time motion extraction from 2D cardiac fat navigator images was feasible within 20 ms, enabling successful prospectively gated coronary magnetic resonance angiographies in all subjects. Compared to 1D diaphragmatic navigator, 2D fat image navigator reduced scan time by 38% (P &lt; 0.0005), and significantly improved vessel sharpness, myocardial suppression, and image quality (P &lt; 0.05).


Conclusion
This demonstrates the feasibility of a 3D SSFP coronary magnetic resonance angiography sequence using a 2D epicardial fat image as a navigator for real-time prospective motion tracking. Magn Reson Med 000:000–000, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24721." xmlns="http://purl.org/rss/1.0/"><title>Accelerated MR diffusion tensor imaging using distributed compressed sensing</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24721.</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Accelerated MR diffusion tensor imaging using distributed compressed sensing</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yin Wu, Yan-Jie Zhu, Qiu-Yang Tang, Chao Zou, Wei Liu, Rui-Bin Dai, Xin Liu, Ed X. Wu, Leslie Ying, Dong Liang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-14T23:50:31.544282-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24721.</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24721.</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24721.</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24721-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Diffusion tensor imaging (DTI) is known to suffer from long acquisition time in the orders of several minutes or even hours. Therefore, a feasible way to accelerate DTI data acquisition is highly desirable. In this article, the feasibility and efficacy of distributed compressed sensing to fast DTI is investigated by exploiting the joint sparsity prior in diffusion-weighted images.</p></div></div>
<div class="section" id="mrm24721-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Fully sampled DTI datasets were obtained from both simulated phantom and experimental heart sample, with diffusion gradient applied in six directions. The k-space data were undersampled retrospectively with acceleration factors from 2 to 6. Diffusion-weighted images were reconstructed by solving an <em>l</em><sub>2</sub>-<em>l</em><sub>1</sub> norm minimization problem. Reconstruction performance with varied signal-to-noise ratio and acceleration factors were evaluated by root-mean-square error and maps of reconstructed DTI indices.</p></div></div>
<div class="section" id="mrm24721-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Superiority of distributed compressed sensing over basic compressed sensing was confirmed with simulation, and the reconstruction accuracy was influenced by signal-to-noise ratio and acceleration factors. Experimental results demonstrate that DTI indices including fractional anisotropy, mean diffusivities, and orientation of primary eigenvector can be obtained with high accuracy at acceleration factors up to 4.</p></div></div>
<div class="section" id="mrm24721-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Distributed compressed sensing is shown to be able to accelerate DTI and may be used to reduce DTI acquisition time practically.</p></div></div>
]]></content:encoded><description>

Purpose
Diffusion tensor imaging (DTI) is known to suffer from long acquisition time in the orders of several minutes or even hours. Therefore, a feasible way to accelerate DTI data acquisition is highly desirable. In this article, the feasibility and efficacy of distributed compressed sensing to fast DTI is investigated by exploiting the joint sparsity prior in diffusion-weighted images.


Methods
Fully sampled DTI datasets were obtained from both simulated phantom and experimental heart sample, with diffusion gradient applied in six directions. The k-space data were undersampled retrospectively with acceleration factors from 2 to 6. Diffusion-weighted images were reconstructed by solving an l2-l1 norm minimization problem. Reconstruction performance with varied signal-to-noise ratio and acceleration factors were evaluated by root-mean-square error and maps of reconstructed DTI indices.


Results
Superiority of distributed compressed sensing over basic compressed sensing was confirmed with simulation, and the reconstruction accuracy was influenced by signal-to-noise ratio and acceleration factors. Experimental results demonstrate that DTI indices including fractional anisotropy, mean diffusivities, and orientation of primary eigenvector can be obtained with high accuracy at acceleration factors up to 4.


Conclusion
Distributed compressed sensing is shown to be able to accelerate DTI and may be used to reduce DTI acquisition time practically.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24718" xmlns="http://purl.org/rss/1.0/"><title>Simultaneous spatial and spectral selectivity by spatiotemporal encoding</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24718</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Simultaneous spatial and spectral selectivity by spatiotemporal encoding</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jean-Nicolas Dumez, Rita Schmidt, Lucio Frydman</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-14T17:43:01.192233-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24718</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24718</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24718</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24718-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To introduce a method that provides simultaneous spatial and spectral selectivity, whose implementation is less demanding than—and quality comparable to—conventional 2D spectral-spatial counterparts.</p></div></div>
<div class="section" id="mrm24718-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory</h4><div class="para"><p>Spatiotemporal encoding concepts lead to a spatially selective, chemical-shift-dependent echo, with simultaneous dephasing of all other off-resonant species. The approach only requires applying a pair of suitable radiofrequency-swept pulses, and allows arbitrary shaping of the spatial profiles.</p></div></div>
<div class="section" id="mrm24718-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Based on arguments derived for chirp pulses operating in the sequential-sweep approximation, quadratic-phase SLR excitation and refocusing waveforms were designed and used to collect 2D slice- and shift-selective images on a 7 T microimaging system (phantoms). The same strategy was used to obtain multi-slice echo-planar and spin-echo images of breast on human volunteers in a 3 T scanner.</p></div></div>
<div class="section" id="mrm24718-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The method managed to deliver excellent shift-selective multi-slice images in phantoms and human volunteers. Simultaneous water and fat images were also collected in a single, interleaved acquisition mode on both platforms, using straightforward sequence and reconstruction modifications of the basic scheme.</p></div></div>
<div class="section" id="mrm24718-sec-0005" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>A new way to achieve chemical shift selectivity with high quality spatial profiling is achieved, without the usual requirements for playing out fast oscillating gradients in conjunction with carefully timed radiofrequency pulses. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To introduce a method that provides simultaneous spatial and spectral selectivity, whose implementation is less demanding than—and quality comparable to—conventional 2D spectral-spatial counterparts.


Theory
Spatiotemporal encoding concepts lead to a spatially selective, chemical-shift-dependent echo, with simultaneous dephasing of all other off-resonant species. The approach only requires applying a pair of suitable radiofrequency-swept pulses, and allows arbitrary shaping of the spatial profiles.


Methods
Based on arguments derived for chirp pulses operating in the sequential-sweep approximation, quadratic-phase SLR excitation and refocusing waveforms were designed and used to collect 2D slice- and shift-selective images on a 7 T microimaging system (phantoms). The same strategy was used to obtain multi-slice echo-planar and spin-echo images of breast on human volunteers in a 3 T scanner.


Results
The method managed to deliver excellent shift-selective multi-slice images in phantoms and human volunteers. Simultaneous water and fat images were also collected in a single, interleaved acquisition mode on both platforms, using straightforward sequence and reconstruction modifications of the basic scheme.


Conclusion
A new way to achieve chemical shift selectivity with high quality spatial profiling is achieved, without the usual requirements for playing out fast oscillating gradients in conjunction with carefully timed radiofrequency pulses. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24693" xmlns="http://purl.org/rss/1.0/"><title>Sparse spectral deconvolution algorithm for noncartesian MR spectroscopic imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24693</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Sparse spectral deconvolution algorithm for noncartesian MR spectroscopic imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sampada Bhave, Ramin Eslami, Mathews Jacob</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-13T07:23:15.074904-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24693</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24693</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24693</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>To minimize line shape distortions and spectral leakage artifacts in MR spectroscopic imaging (MRSI).</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>A spatially and spectrally regularized non-Cartesian MRSI algorithm that uses the line shape distortion priors, estimated from water reference data, to deconvolve the spectra is introduced. Sparse spectral regularization is used to minimize noise amplification associated with deconvolution. A spiral MRSI sequence that heavily oversamples the central k-space regions is used to acquire the MRSI data. The spatial regularization term uses the spatial supports of brain and extracranial fat regions to recover the metabolite spectra and nuisance signals at two different resolutions. Specifically, the nuisance signals are recovered at the maximum resolution to minimize spectral leakage, while the point spread functions of metabolites are controlled to obtain acceptable signal-to-noise ratio.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>The comparisons of the algorithm against Tikhonov regularized reconstructions demonstrates considerably reduced line-shape distortions and improved metabolite maps.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>The proposed sparsity constrained spectral deconvolution scheme is effective in minimizing the line-shape distortions. The dual resolution reconstruction scheme is capable of minimizing spectral leakage artifacts. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
To minimize line shape distortions and spectral leakage artifacts in MR spectroscopic imaging (MRSI).


Methods:
A spatially and spectrally regularized non-Cartesian MRSI algorithm that uses the line shape distortion priors, estimated from water reference data, to deconvolve the spectra is introduced. Sparse spectral regularization is used to minimize noise amplification associated with deconvolution. A spiral MRSI sequence that heavily oversamples the central k-space regions is used to acquire the MRSI data. The spatial regularization term uses the spatial supports of brain and extracranial fat regions to recover the metabolite spectra and nuisance signals at two different resolutions. Specifically, the nuisance signals are recovered at the maximum resolution to minimize spectral leakage, while the point spread functions of metabolites are controlled to obtain acceptable signal-to-noise ratio.


Results:
The comparisons of the algorithm against Tikhonov regularized reconstructions demonstrates considerably reduced line-shape distortions and improved metabolite maps.


Conclusion:
The proposed sparsity constrained spectral deconvolution scheme is effective in minimizing the line-shape distortions. The dual resolution reconstruction scheme is capable of minimizing spectral leakage artifacts. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24726" xmlns="http://purl.org/rss/1.0/"><title>A 16-channel dual-row transmit array in combination with a 31-element receive array for human brain imaging at 9.4 T</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24726</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A 16-channel dual-row transmit array in combination with a 31-element receive array for human brain imaging at 9.4 T</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Shajan, Mikhail Kozlov, Jens Hoffmann, Robert Turner, Klaus Scheffler, Rolf Pohmann</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-11T09:02:41.830699-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24726</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24726</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24726</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24726-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Arranging transmit array elements in multiple rows provides an additional degree of freedom to correct <em>B</em><sub>1</sub><sup>+</sup> field inhomogeneities and to achieve whole-brain excitation at ultrahigh field strengths. Receive arrays shaped to the contours of the anatomy increase the signal-to-noise ratio of the image. In this work, the advantages offered by the transmit and receive array techniques are combined for human brain imaging at 9.4 T.</p></div></div>
<div class="section" id="mrm24726-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A 16-element dual-row transmit array and a 31-element receive array were developed. Based on an accurate numerical model of the transmit array, the deposited power was calculated for different head sizes and positions. The influence of the receive array on the transmit field was characterized. Parallel imaging performance and signal-to-noise ratio of the receive array were evaluated.</p></div></div>
<div class="section" id="mrm24726-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>On average, a two fold increase in signal-to-noise ratio was observed in the whole-brain volume when compared with a 16-channel elliptic microstrip transceiver array. The benefits of combining the two arrays, <em>B</em><sub>1</sub><sup>+</sup> shimming in three directions and high receive sensitivity, are demonstrated with high-resolution in vivo images.</p></div></div>
<div class="section" id="mrm24726-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The dual-row transmit array provides whole-brain coverage at 9.4 T, which, in combination with the helmet-shaped receive array, is a valuable radio frequency configuration for ultra-high field magnetic resonance imaging of the human brain. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Arranging transmit array elements in multiple rows provides an additional degree of freedom to correct B1+ field inhomogeneities and to achieve whole-brain excitation at ultrahigh field strengths. Receive arrays shaped to the contours of the anatomy increase the signal-to-noise ratio of the image. In this work, the advantages offered by the transmit and receive array techniques are combined for human brain imaging at 9.4 T.


Methods
A 16-element dual-row transmit array and a 31-element receive array were developed. Based on an accurate numerical model of the transmit array, the deposited power was calculated for different head sizes and positions. The influence of the receive array on the transmit field was characterized. Parallel imaging performance and signal-to-noise ratio of the receive array were evaluated.


Results
On average, a two fold increase in signal-to-noise ratio was observed in the whole-brain volume when compared with a 16-channel elliptic microstrip transceiver array. The benefits of combining the two arrays, B1+ shimming in three directions and high receive sensitivity, are demonstrated with high-resolution in vivo images.


Conclusion
The dual-row transmit array provides whole-brain coverage at 9.4 T, which, in combination with the helmet-shaped receive array, is a valuable radio frequency configuration for ultra-high field magnetic resonance imaging of the human brain. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24715" xmlns="http://purl.org/rss/1.0/"><title>Pseudometrically constrained centroidal voronoi tessellations: Generating uniform antipodally symmetric points on the unit sphere with a novel acceleration strategy and its applications to diffusion and three-dimensional radial MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24715</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Pseudometrically constrained centroidal voronoi tessellations: Generating uniform antipodally symmetric points on the unit sphere with a novel acceleration strategy and its applications to diffusion and three-dimensional radial MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Cheng Guan Koay</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-11T09:02:31.043703-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24715</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24715</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24715</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24715-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The purpose of this work is to investigate the hypothesis that uniform sampling measurements that are endowed with antipodal symmetry play an important role in image quality when the raw data and image data are related through the Fourier relationship. Currently, it is extremely challenging to generate large and uniform antipodally symmetric point sets suitable for three-dimensional radial MRI. A novel approach is proposed to solve this long-standing problem in a unique and optimal way.</p></div></div>
<div class="section" id="mrm24715-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The proposed method is based on constrained centroidal Voronoi tessellations of the upper hemisphere with a novel pseudometric.</p></div></div>
<div class="section" id="mrm24715-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The time complexity of the proposed tessellations was shown to be effectively linear, i.e., on the order of the number of sampling measurements. For small sample size, the proposed method was comparable with the state-of-the-art method (a direct iterative minimization of the electrostatic potential energy of a collection of electrons antipodal-symmetrically distributed on the unit sphere) in terms of the sampling uniformity. For large sample size, in which the state-of-the-art method is infeasible, the reconstructed images from the proposed method has less streak and ringing artifacts, when compared with those of the commonly used methods.</p></div></div>
<div class="section" id="mrm24715-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>This work proposed a unique and optimal approach to solving a long-standing problem in generating uniform sampling points for three-dimensional radial MRI. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
The purpose of this work is to investigate the hypothesis that uniform sampling measurements that are endowed with antipodal symmetry play an important role in image quality when the raw data and image data are related through the Fourier relationship. Currently, it is extremely challenging to generate large and uniform antipodally symmetric point sets suitable for three-dimensional radial MRI. A novel approach is proposed to solve this long-standing problem in a unique and optimal way.


Methods
The proposed method is based on constrained centroidal Voronoi tessellations of the upper hemisphere with a novel pseudometric.


Results
The time complexity of the proposed tessellations was shown to be effectively linear, i.e., on the order of the number of sampling measurements. For small sample size, the proposed method was comparable with the state-of-the-art method (a direct iterative minimization of the electrostatic potential energy of a collection of electrons antipodal-symmetrically distributed on the unit sphere) in terms of the sampling uniformity. For large sample size, in which the state-of-the-art method is infeasible, the reconstructed images from the proposed method has less streak and ringing artifacts, when compared with those of the commonly used methods.


Conclusion
This work proposed a unique and optimal approach to solving a long-standing problem in generating uniform sampling points for three-dimensional radial MRI. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24704" xmlns="http://purl.org/rss/1.0/"><title>Spectrally resolved fully phase-encoded three-dimensional fast spin-echo imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24704</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Spectrally resolved fully phase-encoded three-dimensional fast spin-echo imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nathan S. Artz, Diego Hernando, Valentina Taviani, Alexey Samsonov, Jean H. Brittain, Scott B. Reeder</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-11T09:02:26.173947-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24704</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24704</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24704</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24704-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To develop and test the feasibility of a spectrally resolved fully phase-encoded (SR-FPE) three-dimensional fast spin-echo technique and to demonstrate its application for distortion-free imaging near metal and chemical species separation.</p></div></div>
<div class="section" id="mrm24704-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>In separate scans at 1.5 T, a hip prosthesis phantom and a sphere filled with gadolinium solution were imaged with SR-FPE and compared to conventional three-dimensional-fast spin-echo. Spectral modeling was performed on the SR-FPE data to generate the following parametric maps: species-specific signal (<em>ρ</em><sub>species</sub>), <em>B</em><sub>0</sub> field inhomogeneity, and R*<sub>2</sub>. The prosthesis phantom was also scanned using a 16-channel coil at 1.5 T. The fully sampled k-space data were retrospectively undersampled to demonstrate the feasibility of parallel imaging acceleration in all three phase-encoding directions, in combination with corner-cutting and half-Fourier sampling. Finally, SR-FPE was performed with an acetone/water/oil phantom to test chemical species separation.</p></div></div>
<div class="section" id="mrm24704-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>High quality distortion-free images and parametric maps were generated from SR-FPE. A 4 h SR-FPE scan was retrospectively accelerated to 12 min while preserving spectral information and 7.5 min without preserving spectral data. Chemical species separation was demonstrated in the acetone/water/oil phantom.</p></div></div>
<div class="section" id="mrm24704-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>This work demonstrates the feasibility of SR-FPE to perform chemical species separation and spectrally resolved imaging near metal without distortion, in scan times appropriate for the clinical setting. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
To develop and test the feasibility of a spectrally resolved fully phase-encoded (SR-FPE) three-dimensional fast spin-echo technique and to demonstrate its application for distortion-free imaging near metal and chemical species separation.


Methods
In separate scans at 1.5 T, a hip prosthesis phantom and a sphere filled with gadolinium solution were imaged with SR-FPE and compared to conventional three-dimensional-fast spin-echo. Spectral modeling was performed on the SR-FPE data to generate the following parametric maps: species-specific signal (ρspecies), B0 field inhomogeneity, and R*2. The prosthesis phantom was also scanned using a 16-channel coil at 1.5 T. The fully sampled k-space data were retrospectively undersampled to demonstrate the feasibility of parallel imaging acceleration in all three phase-encoding directions, in combination with corner-cutting and half-Fourier sampling. Finally, SR-FPE was performed with an acetone/water/oil phantom to test chemical species separation.


Results
High quality distortion-free images and parametric maps were generated from SR-FPE. A 4 h SR-FPE scan was retrospectively accelerated to 12 min while preserving spectral information and 7.5 min without preserving spectral data. Chemical species separation was demonstrated in the acetone/water/oil phantom.


Conclusion
This work demonstrates the feasibility of SR-FPE to perform chemical species separation and spectrally resolved imaging near metal without distortion, in scan times appropriate for the clinical setting. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24650" xmlns="http://purl.org/rss/1.0/"><title>Acceleration-selective arterial spin labeling</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24650</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Acceleration-selective arterial spin labeling</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sophie Schmid, Eidrees Ghariq, Wouter M. Teeuwisse, Andrew Webb, Matthias J. P. Osch</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-08T11:55:35.26018-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24650</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24650</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24650</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>In this study, a new arterial spin labeling (ASL) method with spatially nonselective labeling is introduced, based on the acceleration of flowing spins, which is able to image brain perfusion with minimal contamination from venous signal. This method is termed acceleration-selective ASL (AccASL) and resembles velocity-selective ASL (VSASL), with the difference that AccASL is able to discriminate between arterial and venous components in a single preparation module due to the higher acceleration on the arterial side of the microvasculature, whereas VSASL cannot make this distinction unless a second labeling module is used. A difference between AccASL and VSASL is that AccASL is mainly cerebral blood volume weighted, whereas VSASL is cerebral blood flow weighted. AccASL exploits the principles of acceleration-encoded magnetic resonance angiography by using motion-sensitizing gradients in a <em>T</em><sub>2</sub>-preparation module. This method is demonstrated in healthy volunteers for a range of cutoff accelerations. Additionally, AccASL is compared with VSASL and pseudo-continuous ASL, and its feasibility in functional MRI is demonstrated. Compared with VSASL with a single labeling module, a strong and significant reduction in venous label is observed. The resulting signal-to-noise ratio is comparable to pseudo-continuous ASL and robust activation of the visual cortex is observed. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div>
]]></content:encoded><description>
In this study, a new arterial spin labeling (ASL) method with spatially nonselective labeling is introduced, based on the acceleration of flowing spins, which is able to image brain perfusion with minimal contamination from venous signal. This method is termed acceleration-selective ASL (AccASL) and resembles velocity-selective ASL (VSASL), with the difference that AccASL is able to discriminate between arterial and venous components in a single preparation module due to the higher acceleration on the arterial side of the microvasculature, whereas VSASL cannot make this distinction unless a second labeling module is used. A difference between AccASL and VSASL is that AccASL is mainly cerebral blood volume weighted, whereas VSASL is cerebral blood flow weighted. AccASL exploits the principles of acceleration-encoded magnetic resonance angiography by using motion-sensitizing gradients in a T2-preparation module. This method is demonstrated in healthy volunteers for a range of cutoff accelerations. Additionally, AccASL is compared with VSASL and pseudo-continuous ASL, and its feasibility in functional MRI is demonstrated. Compared with VSASL with a single labeling module, a strong and significant reduction in venous label is observed. The resulting signal-to-noise ratio is comparable to pseudo-continuous ASL and robust activation of the visual cortex is observed. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24717" xmlns="http://purl.org/rss/1.0/"><title>Improved precision in CHARMED assessment of white matter through sampling scheme optimization and model parsimony testing</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24717</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Improved precision in CHARMED assessment of white matter through sampling scheme optimization and model parsimony testing</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. Santis, Y. Assaf, C. J. Evans, D. K. Jones</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-08T11:33:06.289168-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24717</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24717</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24717</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24717-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The composite hindered and restricted model of diffusion provides microstructural indices that are potentially more specific than those from diffusion tensor imaging. However, in comparison to diffusion tensor imaging, the acquisition time is longer, limiting clinical applications. Moreover, the model requires several parameters to be estimated whose confidence intervals can be large. Here, the composite hindered and restricted model of diffusion acquisition and data processing pipelines are optimized to extend the utility of this approach.</p></div></div>
<div class="section" id="mrm24717-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A multishell sampling scheme was optimized using the electrostatic repulsion algorithm, combined with optimal ordering. The optimal protocol, using as few measurements as possible, was determined through leave-<em>n</em>-out analyses. Parsimonious model selection criteria were used to select between nested models, comprising up to three restricted compartments. The schemes were evaluated using both through Monte-Carlo simulations and in vivo data.</p></div></div>
<div class="section" id="mrm24717-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The optimization/model selection procedure resulted in increased accuracy and precision on the estimated parameters, allowing for a reduction in acquisition time and marked improvements in data quality. The final protocol provided whole brain coverage data in only 12 min.</p></div></div>
<div class="section" id="mrm24717-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Through careful optimization of the acquisition and analysis pipeline for the composite hindered and restricted model of diffusion, it is possible to reduce acquisition time for whole brain datasets to a time that is clinically applicable. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The composite hindered and restricted model of diffusion provides microstructural indices that are potentially more specific than those from diffusion tensor imaging. However, in comparison to diffusion tensor imaging, the acquisition time is longer, limiting clinical applications. Moreover, the model requires several parameters to be estimated whose confidence intervals can be large. Here, the composite hindered and restricted model of diffusion acquisition and data processing pipelines are optimized to extend the utility of this approach.


Methods
A multishell sampling scheme was optimized using the electrostatic repulsion algorithm, combined with optimal ordering. The optimal protocol, using as few measurements as possible, was determined through leave-n-out analyses. Parsimonious model selection criteria were used to select between nested models, comprising up to three restricted compartments. The schemes were evaluated using both through Monte-Carlo simulations and in vivo data.


Results
The optimization/model selection procedure resulted in increased accuracy and precision on the estimated parameters, allowing for a reduction in acquisition time and marked improvements in data quality. The final protocol provided whole brain coverage data in only 12 min.


Conclusion
Through careful optimization of the acquisition and analysis pipeline for the composite hindered and restricted model of diffusion, it is possible to reduce acquisition time for whole brain datasets to a time that is clinically applicable. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24720" xmlns="http://purl.org/rss/1.0/"><title>Detecting neuronal currents with MRI: A human study</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24720</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Detecting neuronal currents with MRI: A human study</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jie Huang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-08T11:32:03.002632-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24720</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24720</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24720</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24720-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Recently developed neuronal current magnetic resonance imaging aims to directly detect neuronal currents associated with brain activity, but controversial results have been reported in different studies on human subjects. Although there is no dispute that local neuronal currents produce weak transient magnetic fields that would attenuate local MR signal intensity, there is not yet consensus as to whether this attenuation is detectable with present magnetic resonance imaging techniques. This study investigates the magnitude of neuronal current-induced signal attenuation in human visual cortex.</p></div></div>
<div class="section" id="mrm24720-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory</h4><div class="para"><p>A temporally well-controlled visual stimulation paradigm with a known neuronal firing pattern in monkey visual cortex provides a means of detecting and testing the magnitude of the neuronal current-induced attenuation in neuronal current magnetic resonance imaging.</p></div></div>
<div class="section" id="mrm24720-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Placing a series of acquisition windows to fully cover the entire response duration enables a thorough detection of any detectable MR signal attenuation induced by the stimulus-evoked neuronal currents.</p></div></div>
<div class="section" id="mrm24720-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>No significant neuronal current-induced MR signal attenuation was observed in the putative V1 in any participated subjects.</p></div></div>
<div class="section" id="mrm24720-sec-0005" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The present magnetic resonance imaging technique is not sensitive enough to detect neuronal current-induced MR signal attenuation, and the upper limit of this attenuation was found to be less than 0.07% under the study condition. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Recently developed neuronal current magnetic resonance imaging aims to directly detect neuronal currents associated with brain activity, but controversial results have been reported in different studies on human subjects. Although there is no dispute that local neuronal currents produce weak transient magnetic fields that would attenuate local MR signal intensity, there is not yet consensus as to whether this attenuation is detectable with present magnetic resonance imaging techniques. This study investigates the magnitude of neuronal current-induced signal attenuation in human visual cortex.


Theory
A temporally well-controlled visual stimulation paradigm with a known neuronal firing pattern in monkey visual cortex provides a means of detecting and testing the magnitude of the neuronal current-induced attenuation in neuronal current magnetic resonance imaging.


Methods
Placing a series of acquisition windows to fully cover the entire response duration enables a thorough detection of any detectable MR signal attenuation induced by the stimulus-evoked neuronal currents.


Results
No significant neuronal current-induced MR signal attenuation was observed in the putative V1 in any participated subjects.


Conclusion
The present magnetic resonance imaging technique is not sensitive enough to detect neuronal current-induced MR signal attenuation, and the upper limit of this attenuation was found to be less than 0.07% under the study condition. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24712" xmlns="http://purl.org/rss/1.0/"><title>Uniform spinning sampling gradient electron paramagnetic resonance imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24712</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Uniform spinning sampling gradient electron paramagnetic resonance imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">David H. Johnson, Rizwan Ahmad, Yangping Liu, Zhiyu Chen, Alexandre Samouilov, Jay L. Zweier</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-08T11:31:39.710605-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24712</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24712</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24712</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24712-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To improve the quality and speed of electron paramagnetic resonance imaging (EPRI) acquisition by combining a uniform sampling distribution with spinning gradient acquisition.</p></div></div>
<div class="section" id="mrm24712-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>A uniform sampling distribution was derived for spinning gradient EPRI acquisition (uniform spinning sampling, USS) and compared to the existing (equilinear spinning sampling, ESS) acquisition strategy. Novel corrections were introduced to reduce artifacts in experimental data.</p></div></div>
<div class="section" id="mrm24712-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Simulations demonstrated that USS puts an equal number of projections near each axis whereas ESS puts excessive projections at one axis, wasting acquisition time. Artifact corrections added to the magnetic gradient waveforms reduced noise and correlation between projections. USS images had higher SNR (85.9 ± 0.8 vs. 56.2 ± 0.8) and lower mean-squared error than ESS images. The quality of the USS images did not vary with the magnetic gradient orientation, in contrast to ESS images. The quality of rat heart images was improved using USS compared to that with ESS or traditional fast-scan acquisitions.</p></div></div>
<div class="section" id="mrm24712-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>A novel EPRI acquisition which combines spinning gradient acquisition with a uniform sampling distribution was developed. This USS spinning gradient acquisition offers superior SNR and reduced artifacts compared to prior methods enabling potential improvements in speed and quality of EPR imaging in biological applications. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To improve the quality and speed of electron paramagnetic resonance imaging (EPRI) acquisition by combining a uniform sampling distribution with spinning gradient acquisition.


Theory and Methods
A uniform sampling distribution was derived for spinning gradient EPRI acquisition (uniform spinning sampling, USS) and compared to the existing (equilinear spinning sampling, ESS) acquisition strategy. Novel corrections were introduced to reduce artifacts in experimental data.


Results
Simulations demonstrated that USS puts an equal number of projections near each axis whereas ESS puts excessive projections at one axis, wasting acquisition time. Artifact corrections added to the magnetic gradient waveforms reduced noise and correlation between projections. USS images had higher SNR (85.9 ± 0.8 vs. 56.2 ± 0.8) and lower mean-squared error than ESS images. The quality of the USS images did not vary with the magnetic gradient orientation, in contrast to ESS images. The quality of rat heart images was improved using USS compared to that with ESS or traditional fast-scan acquisitions.


Conclusion
A novel EPRI acquisition which combines spinning gradient acquisition with a uniform sampling distribution was developed. This USS spinning gradient acquisition offers superior SNR and reduced artifacts compared to prior methods enabling potential improvements in speed and quality of EPR imaging in biological applications. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24703" xmlns="http://purl.org/rss/1.0/"><title>ProFit revisited</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24703</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">ProFit revisited</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Alexander Fuchs, Peter Boesiger, Rolf F. Schulte, Anke Henning</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-08T11:31:31.642488-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24703</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24703</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24703</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24703-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>An enhanced version of the ProFit fitting tool was developed and validated to improve the quantification of two-dimensional JRPESS spectroscopic data.</p></div></div>
<div class="section" id="mrm24703-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The proposed enhancements were achieved by flexible organization of prior knowledge, configurations for different situations, the inclusion of measured macromolecular baseline contribution, additional baseline splines and a model-free lineshape based on self-deconvolution. The new software was tested and tuned on simulated data and subsequently applied to in vivo intrasubject and intersubject data.</p></div></div>
<div class="section" id="mrm24703-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Fit results of simulated and acquired spectra show good overall quality suggesting the potential reliable detection of up to 18 metabolites on a 3T system yielding Cramer-Lower-Bounds below 20%.</p></div></div>
<div class="section" id="mrm24703-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The proposed enhanced version of ProFit together with two-dimensional J-resolved spectroscopy offers the opportunity to reliably detect a wide selection of important brain metabolites on 3T. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
An enhanced version of the ProFit fitting tool was developed and validated to improve the quantification of two-dimensional JRPESS spectroscopic data.


Methods
The proposed enhancements were achieved by flexible organization of prior knowledge, configurations for different situations, the inclusion of measured macromolecular baseline contribution, additional baseline splines and a model-free lineshape based on self-deconvolution. The new software was tested and tuned on simulated data and subsequently applied to in vivo intrasubject and intersubject data.


Results
Fit results of simulated and acquired spectra show good overall quality suggesting the potential reliable detection of up to 18 metabolites on a 3T system yielding Cramer-Lower-Bounds below 20%.


Conclusion
The proposed enhanced version of ProFit together with two-dimensional J-resolved spectroscopy offers the opportunity to reliably detect a wide selection of important brain metabolites on 3T. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24694" xmlns="http://purl.org/rss/1.0/"><title>Non-invasive quantification of absolute cerebral blood volume during functional activation applicable to the whole human brain</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24694</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Non-invasive quantification of absolute cerebral blood volume during functional activation applicable to the whole human brain</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Pelin Aksit Ciris, Maolin Qiu, Robert Todd Constable</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-08T11:06:56.03-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24694</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24694</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24694</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24694-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Cerebral blood volume (CBV) changes in many diverse pathologic conditions, and in response to functional challenges along with changes in blood flow, blood oxygenation, and the cerebral metabolic rate of oxygen. The feasibility of a new method for non-invasive quantification of absolute cerebral blood volume that can be applicable to the whole human brain was investigated.</p></div></div>
<div class="section" id="mrm24694-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Multi-slice data were acquired at 3 T using a novel inversion recovery echo planar imaging (IR-EPI) pulse sequence with varying contrast weightings and an efficient rotating slice acquisition order, at rest and during visual activation. A biophysical model was used to estimate absolute cerebral blood volume at rest and during activation, and oxygenation during activation, on data from 13 normal human subjects.</p></div></div>
<div class="section" id="mrm24694-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Cerebral blood volume increased by 21.7% from 6.6 ± 0.8 mL/100 mL of brain parenchyma at rest to 8.0 ± 1.3 mL/100 mL of brain parenchyma in the occipital cortex during visual activation, with average blood oxygenation of 84 ± 2.1% during activation, comparing well with literature.</p></div></div>
<div class="section" id="mrm24694-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The method is feasible, and could foster improved understanding of the fundamental physiological relationship between neuronal activity, hemodynamic changes, and metabolism underlying brain activation; complement existing methods for estimating compartmental changes; and potentially find utility in evaluating vascular health. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Cerebral blood volume (CBV) changes in many diverse pathologic conditions, and in response to functional challenges along with changes in blood flow, blood oxygenation, and the cerebral metabolic rate of oxygen. The feasibility of a new method for non-invasive quantification of absolute cerebral blood volume that can be applicable to the whole human brain was investigated.


Methods
Multi-slice data were acquired at 3 T using a novel inversion recovery echo planar imaging (IR-EPI) pulse sequence with varying contrast weightings and an efficient rotating slice acquisition order, at rest and during visual activation. A biophysical model was used to estimate absolute cerebral blood volume at rest and during activation, and oxygenation during activation, on data from 13 normal human subjects.


Results
Cerebral blood volume increased by 21.7% from 6.6 ± 0.8 mL/100 mL of brain parenchyma at rest to 8.0 ± 1.3 mL/100 mL of brain parenchyma in the occipital cortex during visual activation, with average blood oxygenation of 84 ± 2.1% during activation, comparing well with literature.


Conclusion
The method is feasible, and could foster improved understanding of the fundamental physiological relationship between neuronal activity, hemodynamic changes, and metabolism underlying brain activation; complement existing methods for estimating compartmental changes; and potentially find utility in evaluating vascular health. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24705" xmlns="http://purl.org/rss/1.0/"><title>High speed 3D overhauser-enhanced MRI using combined b-SSFP and compressed sensing</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24705</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High speed 3D overhauser-enhanced MRI using combined b-SSFP and compressed sensing</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mathieu Sarracanie, Brandon D. Armstrong, Jason Stockmann, Matthew S. Rosen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-08T11:04:29.772522-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24705</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24705</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24705</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24705-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Overhauser-enhanced MRI is a promising technique for imaging the distribution and dynamics of free radicals. A key challenge for Overhauser-enhanced MRI is attaining high spatial and temporal resolution while simultaneously limiting resonator and sample heating due to the long, high power radio-frequency pulses needed to saturate the electron resonance.</p></div></div>
<div class="section" id="mrm24705-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The approach presented here embeds EPR pulses within a balanced steady state free precession sequence. Unlike other Overhauser-enhanced MRI methods, no separate Overhauser prepolarization step is required. This steady-state approach also eliminates the problem of time-varying Overhauser-enhanced signal and provides constant polarization in the sample during the acquisition. A further increase in temporal resolution was achieved by incorporating undersampled k-space strategies and compressed sensing reconstruction.</p></div></div>
<div class="section" id="mrm24705-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>We demonstrate 1 × 2 × 3.5 mm<sup>3</sup> resolution at 6.5 mT across a 54 × 54 × 110 mm<sup>3</sup> sample in 33 s while sampling 30% of k-space.</p></div></div>
<div class="section" id="mrm24705-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The work presented here overcomes the main limitations of Overhauser enhanced MRI as previously described in the literature, drastically improving speed and resolution, and enabling new opportunities for the measurement of free radicals in living organisms, and for the study of dynamic processes such as metabolism and flow. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Overhauser-enhanced MRI is a promising technique for imaging the distribution and dynamics of free radicals. A key challenge for Overhauser-enhanced MRI is attaining high spatial and temporal resolution while simultaneously limiting resonator and sample heating due to the long, high power radio-frequency pulses needed to saturate the electron resonance.


Methods
The approach presented here embeds EPR pulses within a balanced steady state free precession sequence. Unlike other Overhauser-enhanced MRI methods, no separate Overhauser prepolarization step is required. This steady-state approach also eliminates the problem of time-varying Overhauser-enhanced signal and provides constant polarization in the sample during the acquisition. A further increase in temporal resolution was achieved by incorporating undersampled k-space strategies and compressed sensing reconstruction.


Results
We demonstrate 1 × 2 × 3.5 mm3 resolution at 6.5 mT across a 54 × 54 × 110 mm3 sample in 33 s while sampling 30% of k-space.


Conclusion
The work presented here overcomes the main limitations of Overhauser enhanced MRI as previously described in the literature, drastically improving speed and resolution, and enabling new opportunities for the measurement of free radicals in living organisms, and for the study of dynamic processes such as metabolism and flow. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24699" xmlns="http://purl.org/rss/1.0/"><title>
R2*-corrected water–fat imaging using compressed sensing and parallel imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24699</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">
R2*-corrected water–fat imaging using compressed sensing and parallel imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Curtis N. Wiens, Colin M. McCurdy, Jacob D. Willig-Onwuachi, Charles A. McKenzie</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-08T10:54:49.967773-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24699</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24699</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24699</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24699-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To demonstrate an approach to water–fat separation with 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24699/asset/equation/mrm24699-math-0002.gif?v=1&amp;t=hh1lk45w&amp;s=d4330813a1012cd7a91cb4b4dcaa828bd3cbca9c" class="inlineGraphic"/> correction using compressed sensing and parallel imaging.</p></div></div>
<div class="section" id="mrm24699-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Acquisition times for chemical shift based water–fat separation imaging are lengthy, and many applications rely on image acceleration techniques. In this study, we present an integrated compressed sensing, parallel imaging, 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24699/asset/equation/mrm24699-math-0003.gif?v=1&amp;t=hh1lk45x&amp;s=1891206db8b966293fb6fcdef961a6cf727fc612" class="inlineGraphic"/> corrected water–fat separation technique for water–fat imaging of highly accelerated acquisitions. Reconstruction times are reduced using coil compression.</p></div></div>
<div class="section" id="mrm24699-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The proposed technique is demonstrated using a customized IDEAL-SPGR pulse sequence to acquire retrospectively and prospectively undersampled datasets of the liver, calf, knee, and abdominal cavity. This technique is shown to offer comparable image quality relative to fully sampled reference images for a range of acceleration factors. At high acceleration factors, this technique is shown to offer improved image quality over parallel imaging.</p></div></div>
<div class="section" id="mrm24699-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>A technique is described that uses compressed sensing and parallel imaging to reconstruct 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24699/asset/equation/mrm24699-math-0004.gif?v=1&amp;t=hh1lk45y&amp;s=58863b96601ac27b6af41e9068941bc6a68c42ea" class="inlineGraphic"/>-corrected water and fat images from accelerated datasets. Acceleration factors as high as 7.0 are shown with excellent image quality. These high acceleration factors enable water–fat separation with higher resolution or greater anatomical coverage in breath-hold applications. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To demonstrate an approach to water–fat separation with 
R2* correction using compressed sensing and parallel imaging.


Methods
Acquisition times for chemical shift based water–fat separation imaging are lengthy, and many applications rely on image acceleration techniques. In this study, we present an integrated compressed sensing, parallel imaging, 
R2* corrected water–fat separation technique for water–fat imaging of highly accelerated acquisitions. Reconstruction times are reduced using coil compression.


Results
The proposed technique is demonstrated using a customized IDEAL-SPGR pulse sequence to acquire retrospectively and prospectively undersampled datasets of the liver, calf, knee, and abdominal cavity. This technique is shown to offer comparable image quality relative to fully sampled reference images for a range of acceleration factors. At high acceleration factors, this technique is shown to offer improved image quality over parallel imaging.


Conclusion
A technique is described that uses compressed sensing and parallel imaging to reconstruct 
R2*-corrected water and fat images from accelerated datasets. Acceleration factors as high as 7.0 are shown with excellent image quality. These high acceleration factors enable water–fat separation with higher resolution or greater anatomical coverage in breath-hold applications. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24707" xmlns="http://purl.org/rss/1.0/"><title>Use of a computer-controlled motion phantom to investigate the temporal and spatial fidelity of HYPR processing</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24707</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Use of a computer-controlled motion phantom to investigate the temporal and spatial fidelity of HYPR processing</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lauren Keith, Mahdi Rahimi, James Holmes, Jean Brittain, Frank Korosec</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-08T10:54:38.283417-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24707</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24707</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24707</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24707-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>In this work, we investigate the spatial and temporal fidelity of highly constrained backPRojection (HYPR) processing using a computer-controlled motion phantom. The goal of this experimental set-up was to provide not only well-defined temporal dynamics and spatial characteristics of the motion phantom, but also circumstances that imitate in vivo scenarios.</p></div></div>
<div class="section" id="mrm24707-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The phantom was designed to represent an artery flanked on both sides by vein. Both arterial and venous components have different temporal dynamics but are confluent, which corresponds to a difficult scenario for HYPR. Spatial and temporal fidelity was investigated by measuring signal intensity profiles through the phantom both orthogonal to as well as along the direction of motion.</p></div></div>
<div class="section" id="mrm24707-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Spatial fidelity profiles measured from the HYPR processed images yielded full-width-at-half-maximum values very similar to those measured in non-HYPR-processed images. Furthermore, there was no significant spreading of the motion phantom leading edge in HYPR processed images.</p></div></div>
<div class="section" id="mrm24707-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Although HYPR processing has certain characteristic artifacts that are discussed, the technique can be used to improve image quality of highly undersampled time frame images with minimal loss of spatial or temporal fidelity. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
In this work, we investigate the spatial and temporal fidelity of highly constrained backPRojection (HYPR) processing using a computer-controlled motion phantom. The goal of this experimental set-up was to provide not only well-defined temporal dynamics and spatial characteristics of the motion phantom, but also circumstances that imitate in vivo scenarios.


Methods
The phantom was designed to represent an artery flanked on both sides by vein. Both arterial and venous components have different temporal dynamics but are confluent, which corresponds to a difficult scenario for HYPR. Spatial and temporal fidelity was investigated by measuring signal intensity profiles through the phantom both orthogonal to as well as along the direction of motion.


Results
Spatial fidelity profiles measured from the HYPR processed images yielded full-width-at-half-maximum values very similar to those measured in non-HYPR-processed images. Furthermore, there was no significant spreading of the motion phantom leading edge in HYPR processed images.


Conclusion
Although HYPR processing has certain characteristic artifacts that are discussed, the technique can be used to improve image quality of highly undersampled time frame images with minimal loss of spatial or temporal fidelity. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24635" xmlns="http://purl.org/rss/1.0/"><title>In vivo 1H MR spectroscopic imaging of aggressive prostate cancer: Can we detect lactate?</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24635</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">In vivo 1H MR spectroscopic imaging of aggressive prostate cancer: Can we detect lactate?</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Thiele Kobus, Alan J. Wright, Jack J. A. Asten, Arend Heerschap, Tom W. J. Scheenen</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-08T10:33:40.238972-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24635</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24635</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24635</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24638-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>A semi-LASER sequence was optimized for in vivo lactate detection in the prostate.</p></div></div>
<div class="section" id="mrm24638-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The ethical committee waived the need for informed consent to measure 17 patients with high grade prostate cancer on a 3T system. A semi-LASER sequence was used with an echo time of 144 ms and optimized interpulse timing for a spectral citrate shape with high signal intensity. An LCModel basis set was developed for fitting choline, creatine, spermine, citrate, and lactate and was used to fit all spectra in tumor-containing voxels. For patients without detectable lactate, the minimal detectable lactate concentration was determined by adding in all spectra of tumor tissue a simulated lactate signal. The amplitude of the simulated lactate signal was iteratively decreased until its fit reached a Cramér Rao lower bound &gt;20%, which was then set as the patient-specific detection limit.</p></div></div>
<div class="section" id="mrm24638-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>In none of the patients a convincing lactate signal was found. We estimated that on average the lactate levels in high grade prostate cancer are below 1.5 mM (range 0.9–3.5 mM), Interestingly, in one patient with extensive necrosis in the tumor biopsy samples (Gleason score 5+5), large lipid resonances were observed, which originated from the tumor.</p></div></div>
<div class="section" id="mrm24638-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The minimal detectable lactate concentration of 1.5 mM in high grade prostate cancer indicates that if lactate is increased it remains at low concentrations. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
A semi-LASER sequence was optimized for in vivo lactate detection in the prostate.


Methods
The ethical committee waived the need for informed consent to measure 17 patients with high grade prostate cancer on a 3T system. A semi-LASER sequence was used with an echo time of 144 ms and optimized interpulse timing for a spectral citrate shape with high signal intensity. An LCModel basis set was developed for fitting choline, creatine, spermine, citrate, and lactate and was used to fit all spectra in tumor-containing voxels. For patients without detectable lactate, the minimal detectable lactate concentration was determined by adding in all spectra of tumor tissue a simulated lactate signal. The amplitude of the simulated lactate signal was iteratively decreased until its fit reached a Cramér Rao lower bound &gt;20%, which was then set as the patient-specific detection limit.


Results
In none of the patients a convincing lactate signal was found. We estimated that on average the lactate levels in high grade prostate cancer are below 1.5 mM (range 0.9–3.5 mM), Interestingly, in one patient with extensive necrosis in the tumor biopsy samples (Gleason score 5+5), large lipid resonances were observed, which originated from the tumor.


Conclusion
The minimal detectable lactate concentration of 1.5 mM in high grade prostate cancer indicates that if lactate is increased it remains at low concentrations. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24668" xmlns="http://purl.org/rss/1.0/"><title>Estimation of single-kidney glomerular filtration rate without exogenous contrast agent</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24668</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Estimation of single-kidney glomerular filtration rate without exogenous contrast agent</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Xiang He, Ayaz Aghayev, Serter Gumus, K. Ty Bae</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-06T12:59:21.889609-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24668</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24668</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24668</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24668-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Measurement of single-kidney filtration fraction and glomerular filtration rate (GFR) without exogenous contrast is clinically important to assess renal function and pathophysiology, especially for patients with comprised renal function. The objective of this study is to develop a novel MR-based tool for noninvasive quantification of renal function using conventional MR arterial spin labeling water as endogenous tracer.</p></div></div>
<div class="section" id="mrm24639-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>The regional differentiation of the arterial spin labeling water between the glomerular capsular space and the renal parenchyma was characterized and measured according to their MR relaxation properties (<em>T</em><sub>1ρ</sub> or <em>T</em><sub>2</sub>), and applied to the estimation of filtration fraction and single-kidney GFR. The proposed approach was tested to quantify GFR in healthy volunteers at baseline and after a protein-loading challenge.</p></div></div>
<div class="section" id="mrm24639-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Biexponential decay of the cortical arterial spin labeling water MR signal was observed. The major component decays the same as parenchyma water; the minor component decays much slower as expected from glomerular ultra-filtrates. The mean single-kidney GFR was estimated to be 49 ± 9 mL/min at baseline and increased by 28% after a protein-loading challenge.</p></div></div>
<div class="section" id="mrm24639-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>We developed an arterial spin labeling-based MR imaging method that allows us to estimate renal filtration fraction and singe-kidney GFR without use of exogenous contrast. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Measurement of single-kidney filtration fraction and glomerular filtration rate (GFR) without exogenous contrast is clinically important to assess renal function and pathophysiology, especially for patients with comprised renal function. The objective of this study is to develop a novel MR-based tool for noninvasive quantification of renal function using conventional MR arterial spin labeling water as endogenous tracer.


Theory and Methods
The regional differentiation of the arterial spin labeling water between the glomerular capsular space and the renal parenchyma was characterized and measured according to their MR relaxation properties (T1ρ or T2), and applied to the estimation of filtration fraction and single-kidney GFR. The proposed approach was tested to quantify GFR in healthy volunteers at baseline and after a protein-loading challenge.


Results
Biexponential decay of the cortical arterial spin labeling water MR signal was observed. The major component decays the same as parenchyma water; the minor component decays much slower as expected from glomerular ultra-filtrates. The mean single-kidney GFR was estimated to be 49 ± 9 mL/min at baseline and increased by 28% after a protein-loading challenge.


Conclusion
We developed an arterial spin labeling-based MR imaging method that allows us to estimate renal filtration fraction and singe-kidney GFR without use of exogenous contrast. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24603" xmlns="http://purl.org/rss/1.0/"><title>In vivo imaging of paraCEST agents using frequency labeled exchange transfer MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24603</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">In vivo imaging of paraCEST agents using frequency labeled exchange transfer MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Chien-Yuan Lin, Nirbhay N. Yadav, James Ratnakar, A. Dean Sherry, Peter C. M. Zijl</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-06T12:17:59.850443-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24603</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24603</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24603</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24603-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>A main obstacle to in vivo applications of paramagnetic chemical exchange saturation transfer (paraCEST) is interference from endogenous tissue magnetization transfer contrast (MTC). The suitability of excitation-based frequency labeled exchange transfer (FLEX) to separate out such MTC effects in vivo was tested.</p></div></div>
<div class="section" id="mrm24603-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The FLEX sequence measures modulation of the water signal based on the chemical shift evolution of solute proton magnetization as a function of evolution time. Time-domain analysis of this water signal allows identification of different solute components and provides a mechanism to separate out the rapidly decaying MTC components with short effective transverse relaxation time (
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24603/asset/equation/mrm24603-math-0001.gif?v=1&amp;t=hh1lk46g&amp;s=5dd3c13828cabc0bcc7920db105869ec2d981189" class="inlineGraphic"/>) values.</p></div></div>
<div class="section" id="mrm24603-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>FLEX imaging of paraCEST agents was possible in vitro in phantoms and in vivo in mouse kidneys and bladder. The results demonstrated that FLEX is capable of separating out the MTC signal from tissues in vivo while providing a quantitative exchange rate for the rapidly exchanging paraCEST water protons by fitting the FLEX time-domain signal to FLEX theory.</p></div></div>
<div class="section" id="mrm24603-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>The first in vivo FLEX images of a paraCEST agent were acquired, which allowed separation of the tissue MTC components. These results show that FLEX imaging has potential for imaging the distribution of functional paraCEST agents in biological tissues. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
A main obstacle to in vivo applications of paramagnetic chemical exchange saturation transfer (paraCEST) is interference from endogenous tissue magnetization transfer contrast (MTC). The suitability of excitation-based frequency labeled exchange transfer (FLEX) to separate out such MTC effects in vivo was tested.


Methods
The FLEX sequence measures modulation of the water signal based on the chemical shift evolution of solute proton magnetization as a function of evolution time. Time-domain analysis of this water signal allows identification of different solute components and provides a mechanism to separate out the rapidly decaying MTC components with short effective transverse relaxation time (
T2*) values.


Results
FLEX imaging of paraCEST agents was possible in vitro in phantoms and in vivo in mouse kidneys and bladder. The results demonstrated that FLEX is capable of separating out the MTC signal from tissues in vivo while providing a quantitative exchange rate for the rapidly exchanging paraCEST water protons by fitting the FLEX time-domain signal to FLEX theory.


Conclusions
The first in vivo FLEX images of a paraCEST agent were acquired, which allowed separation of the tissue MTC components. These results show that FLEX imaging has potential for imaging the distribution of functional paraCEST agents in biological tissues. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24670" xmlns="http://purl.org/rss/1.0/"><title>Myelin water mapping by spatially regularized longitudinal relaxographic imaging at high magnetic fields</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24670</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Myelin water mapping by spatially regularized longitudinal relaxographic imaging at high magnetic fields</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Christian Labadie, Jing-Huei Lee, William D. Rooney, Silvia Jarchow, Monique Aubert-Frécon, Charles S. Springer, Harald E. Möller</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-06T10:47:53.895117-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24670</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24670</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24670</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24670-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Magnetic resonance <em>T</em><sub>1</sub>-weighted images are routinely used for human brain segmentation, brain parcellation, and clinical diagnosis of demyelinating diseases. Myelin is thought to influence the longitudinal relaxation commonly described by a mono-exponential recovery, although reports of bi-exponential longitudinal relaxation have been published. The purpose of this work was to investigate if a myelin water <em>T</em><sub>1</sub> contribution could be separated in geometrically sampled Look-Locker trains of low flip angle gradient echoes.</p></div></div>
<div class="section" id="mrm24670-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p><em>T</em><sub>1</sub> relaxograms from normal human brain were computed by a spatially regularized inverse Laplace transform after estimating the apparent inversion efficiency.</p></div></div>
<div class="section" id="mrm24670-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>With sufficiently long inversion-time sampling (ca. 5 × <em>T</em><sub>1</sub> of cerebrospinal fluid), the <em>T</em><sub>1</sub> relaxogram revealed a short-<em>T</em><sub>1</sub> peak (106–225 ms). The apparent fraction of this water component increased in human brain white matter from 8.3% at 3 T, to 11.3% at 4 T and 15.0% at 7 T. The <em>T</em><sub>2</sub>* of the short-<em>T</em><sub>1</sub> peak at 3 T was shorter, 27.9 ± 13.0 ms, than that of the long-<em>T</em><sub>1</sub> peak, 51.3 ± 5.6 ms.</p></div></div>
<div class="section" id="mrm24670-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The short-<em>T</em><sub>1</sub> fraction is interpreted as the water resident in myelin. Its detection is facilitated by longer <em>T</em><sub>1</sub> of axoplasmic water at higher magnetic field. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Magnetic resonance T1-weighted images are routinely used for human brain segmentation, brain parcellation, and clinical diagnosis of demyelinating diseases. Myelin is thought to influence the longitudinal relaxation commonly described by a mono-exponential recovery, although reports of bi-exponential longitudinal relaxation have been published. The purpose of this work was to investigate if a myelin water T1 contribution could be separated in geometrically sampled Look-Locker trains of low flip angle gradient echoes.


Methods
T1 relaxograms from normal human brain were computed by a spatially regularized inverse Laplace transform after estimating the apparent inversion efficiency.


Results
With sufficiently long inversion-time sampling (ca. 5 × T1 of cerebrospinal fluid), the T1 relaxogram revealed a short-T1 peak (106–225 ms). The apparent fraction of this water component increased in human brain white matter from 8.3% at 3 T, to 11.3% at 4 T and 15.0% at 7 T. The T2* of the short-T1 peak at 3 T was shorter, 27.9 ± 13.0 ms, than that of the long-T1 peak, 51.3 ± 5.6 ms.


Conclusion
The short-T1 fraction is interpreted as the water resident in myelin. Its detection is facilitated by longer T1 of axoplasmic water at higher magnetic field. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24701" xmlns="http://purl.org/rss/1.0/"><title>Intramolecular zero-quantum-coherence 2D NMR spectroscopy of lipids in the human breast at 7 T</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24701</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Intramolecular zero-quantum-coherence 2D NMR spectroscopy of lipids in the human breast at 7 T</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Robin A. Graaf, Dennis W. J. Klomp, Peter R. Luijten, Vincent O. Boer</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-06T10:30:28.81762-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24701</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24701</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24701</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24701-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Intramolecular zero-quantum-coherences (ZQCs) are intrinsically insensitive toward magnetic field inhomogeneity. This fact is used to quantify and characterize lipid signals in the human breast at 7 T despite the presence of severe magnetic field inhomogeneity caused by water–lipid susceptibility boundaries.</p></div></div>
<div class="section" id="mrm24701-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A novel 3D localized 2D ZQC method is presented. The combination of cardiac/respiratory triggering and post-acquisition navigator echo correction provides high-quality 2D NMR spectra in vivo.</p></div></div>
<div class="section" id="mrm24701-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The lipid profile of the human breast could be quantified by 2D ZQC NMR in 100% of the subjects despite a wide range of magnetic field homogeneity. With conventional 1D <sup>1</sup>H MRS, the magnetic field homogeneity was only adequate in 60% of the subjects. The results from 2D ZQC NMR and 1D NMR are in good correspondence, both in vitro and in vivo.</p></div></div>
<div class="section" id="mrm24701-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>It has been demonstrated that high quality and quantitative 2D ZQC NMR spectra can be acquired from human breast tissue at 7 T. While the simplicity and sensitivity of 1D MRS are preferable when the magnetic field homogeneity is adequate, the 2D ZQC method provides a viable alternative in cases where this requirement cannot be met. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Intramolecular zero-quantum-coherences (ZQCs) are intrinsically insensitive toward magnetic field inhomogeneity. This fact is used to quantify and characterize lipid signals in the human breast at 7 T despite the presence of severe magnetic field inhomogeneity caused by water–lipid susceptibility boundaries.


Methods
A novel 3D localized 2D ZQC method is presented. The combination of cardiac/respiratory triggering and post-acquisition navigator echo correction provides high-quality 2D NMR spectra in vivo.


Results
The lipid profile of the human breast could be quantified by 2D ZQC NMR in 100% of the subjects despite a wide range of magnetic field homogeneity. With conventional 1D 1H MRS, the magnetic field homogeneity was only adequate in 60% of the subjects. The results from 2D ZQC NMR and 1D NMR are in good correspondence, both in vitro and in vivo.


Conclusion
It has been demonstrated that high quality and quantitative 2D ZQC NMR spectra can be acquired from human breast tissue at 7 T. While the simplicity and sensitivity of 1D MRS are preferable when the magnetic field homogeneity is adequate, the 2D ZQC method provides a viable alternative in cases where this requirement cannot be met. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24708" xmlns="http://purl.org/rss/1.0/"><title>Automatic detection of small bowel contraction frequencies in motility plots using lomb-scargle periodogram and sinus-fitting method—initial experience</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24708</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Automatic detection of small bowel contraction frequencies in motility plots using lomb-scargle periodogram and sinus-fitting method—initial experience</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sebastian Bickelhaupt, Roger Cattin, Johannes M. Froehlich, Stephan Raible, Hanspeter Bouquet, Urs Bill, Michael A. Patak</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-06T10:28:53.034682-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24708</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24708</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24708</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24708-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Contraction frequencies are an important parameter for the analysis of bowel motility in MRI. The contraction curve can be rather noisy and the frequency-evaluation might be difficult. The aim was to evaluate manual calculations of small bowel contraction frequency in comparison with automatic calculations using two mathematically established methods.</p></div></div>
<div class="section" id="mrm24708-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The institutional-review-board approved study consisted of 48 segmental small-bowel motility-plots out of a previous study with 25 patients (15 men/10 women; mean 39 years, standard deviation ± 14.67) undergoing MRI (1.5 T, GE-Medical Systems; two-dimensional-Fiesta, pulse repetition time 2.91, echo time 1.25, flip-angle 45°, matrix 256 × 256, slice thickness 10 mm) were evaluated. Calculations of contraction frequency was performed either manually or using Lomb-Scargle-periodograms and Sinus-Fitting method. The results were compared using intraclass correlation coefficient, Friedman's-test and Wilcoxon-matched-paired-signed-rank-test (<em>P</em> &lt; 0.05 considered statistically significant).</p></div></div>
<div class="section" id="mrm24708-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Mean contraction frequency was 5.69 (standard deviation ± 1.99) for manual calculations showing moderate interreader reliability (intraclass correlation coefficient 0.72; 95% confidence-interval: 0.59;0.82). No significant difference (<em>P</em> = 0.776) was found to Lomb-Scargle-periodograms (5.34 contractions-per-minute [cpm], standard deviation ± 2.47; <em>P</em> = 0.174) and to the sinus-fitting-method (5.47 cpm; standard deviation ± 2.57; <em>P</em> = 0.0779). For the latter calculations failed in 3/48 plots, while manual and Lomb-Scargle-periodograms could be performed successfully in all 48/48 plots.</p></div></div>
<div class="section" id="mrm24708-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Herein, we could show that Lomb-Scargle-periodograms and Sinus-Fitting are fast and reliable methods to automatically measure small-bowel contraction frequencies even in noisy small bowel motility plots. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Contraction frequencies are an important parameter for the analysis of bowel motility in MRI. The contraction curve can be rather noisy and the frequency-evaluation might be difficult. The aim was to evaluate manual calculations of small bowel contraction frequency in comparison with automatic calculations using two mathematically established methods.


Methods
The institutional-review-board approved study consisted of 48 segmental small-bowel motility-plots out of a previous study with 25 patients (15 men/10 women; mean 39 years, standard deviation ± 14.67) undergoing MRI (1.5 T, GE-Medical Systems; two-dimensional-Fiesta, pulse repetition time 2.91, echo time 1.25, flip-angle 45°, matrix 256 × 256, slice thickness 10 mm) were evaluated. Calculations of contraction frequency was performed either manually or using Lomb-Scargle-periodograms and Sinus-Fitting method. The results were compared using intraclass correlation coefficient, Friedman's-test and Wilcoxon-matched-paired-signed-rank-test (P &lt; 0.05 considered statistically significant).


Results
Mean contraction frequency was 5.69 (standard deviation ± 1.99) for manual calculations showing moderate interreader reliability (intraclass correlation coefficient 0.72; 95% confidence-interval: 0.59;0.82). No significant difference (P = 0.776) was found to Lomb-Scargle-periodograms (5.34 contractions-per-minute [cpm], standard deviation ± 2.47; P = 0.174) and to the sinus-fitting-method (5.47 cpm; standard deviation ± 2.57; P = 0.0779). For the latter calculations failed in 3/48 plots, while manual and Lomb-Scargle-periodograms could be performed successfully in all 48/48 plots.


Conclusion
Herein, we could show that Lomb-Scargle-periodograms and Sinus-Fitting are fast and reliable methods to automatically measure small-bowel contraction frequencies even in noisy small bowel motility plots. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24713" xmlns="http://purl.org/rss/1.0/"><title>Direct radiofrequency phase control in MRI by digital waveform playback at the larmor frequency</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24713</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Direct radiofrequency phase control in MRI by digital waveform playback at the larmor frequency</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Andrzej Jesmanowicz, Andrew Nencka, James S. Hyde</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-06T10:25:36.286805-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24713</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24713</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24713</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24713-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>A scalable multiband and multichannel digital magnetic resonance imaging system has been developed with the goal of reducing the time needed for acquisition of a single volume of gradient-recalled echo-planar images of the brain.</p></div></div>
<div class="section" id="mrm24713-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Transmit pulses are created by an offline computer equipped with a Pentek excitation card (PCIe model 78621) that was built around the Texas Instruments D/A converter (DAC5688).</p></div></div>
<div class="section" id="mrm24713-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The spectral purity of pulses made in this way surpasses the quality of pulses made by the standard modulators of the scanner, even when using the same pulse-creation algorithm. There is no need to mix reference waveforms with the magnetic resonance imaging signal to obtain inter-k-space coherency for different repetitions. The key was the use of a system clock to create the Larmor frequency used for pulse formation. The 3- and 4-fold slice accelerations were tested using phantoms as well as functional and resting-state magnetic resonance imaging of the human brain.</p></div></div>
<div class="section" id="mrm24713-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Synthesizers with limited modulation-time steps should be replaced not only because of the improved spectral quality of radiofrequency pulses but also for the exceptional coherence of pulses at different slice-selection frequencies. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
A scalable multiband and multichannel digital magnetic resonance imaging system has been developed with the goal of reducing the time needed for acquisition of a single volume of gradient-recalled echo-planar images of the brain.


Methods
Transmit pulses are created by an offline computer equipped with a Pentek excitation card (PCIe model 78621) that was built around the Texas Instruments D/A converter (DAC5688).


Results
The spectral purity of pulses made in this way surpasses the quality of pulses made by the standard modulators of the scanner, even when using the same pulse-creation algorithm. There is no need to mix reference waveforms with the magnetic resonance imaging signal to obtain inter-k-space coherency for different repetitions. The key was the use of a system clock to create the Larmor frequency used for pulse formation. The 3- and 4-fold slice accelerations were tested using phantoms as well as functional and resting-state magnetic resonance imaging of the human brain.


Conclusion
Synthesizers with limited modulation-time steps should be replaced not only because of the improved spectral quality of radiofrequency pulses but also for the exceptional coherence of pulses at different slice-selection frequencies. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24714" xmlns="http://purl.org/rss/1.0/"><title>New spatiotemporal approaches for fully refocused, multislice ultrafast 2D MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24714</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">New spatiotemporal approaches for fully refocused, multislice ultrafast 2D MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rita Schmidt, Lucio Frydman</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-06T10:24:30.622937-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24714</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24714</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24714</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24714-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Single-scan multislice acquisition schemes play key roles in magnetic resonance imaging. Central among these “ultrafast” experiments stands echo-planar imaging, a technique that although of optimal sampling is challenged by <em>T</em><sub>2</sub>* artifacts. Recent studies described alternatives based on spatiotemporal encoding (SPEN), which are particularly robust if implemented in a “full-refocusing” mode. This work extends this modality from the single-slice acquisitions in which it has hitherto been implemented, by introducing a variety of multislice schemes scanning 3D volumes.</p></div></div>
<div class="section" id="mrm24714-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Multislice SPEN employing either inversion or stimulated echo pulses and timed to fulfill the demands of full refocusing, are demonstrated. The performance of the ensuing methods was examined in “Hybrid” modalities encoding data in k- and direct-space, in low-specific absorption rate stimulated-echo approaches, and in direct-space SPEN approaches.</p></div></div>
<div class="section" id="mrm24714-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>When applied in phantoms and in in vivo systems, the ensuing single-shot sequences evidenced similar robustness, sensitivity, and resolution qualities as previously discussed 2D single-slice schemes, while enabling a rapid sampling of the third dimension via multislicing.</p></div></div>
<div class="section" id="mrm24714-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The unique benefits deriving from fully refocused, multislice, single-scan SPEN sequences were corroborated by phantom tests, as well as by in vivo scans at 3 and 7 T. Low specific absorption rate multislice SPEN variants compatible with human studies were demonstrated. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Single-scan multislice acquisition schemes play key roles in magnetic resonance imaging. Central among these “ultrafast” experiments stands echo-planar imaging, a technique that although of optimal sampling is challenged by T2* artifacts. Recent studies described alternatives based on spatiotemporal encoding (SPEN), which are particularly robust if implemented in a “full-refocusing” mode. This work extends this modality from the single-slice acquisitions in which it has hitherto been implemented, by introducing a variety of multislice schemes scanning 3D volumes.


Methods
Multislice SPEN employing either inversion or stimulated echo pulses and timed to fulfill the demands of full refocusing, are demonstrated. The performance of the ensuing methods was examined in “Hybrid” modalities encoding data in k- and direct-space, in low-specific absorption rate stimulated-echo approaches, and in direct-space SPEN approaches.


Results
When applied in phantoms and in in vivo systems, the ensuing single-shot sequences evidenced similar robustness, sensitivity, and resolution qualities as previously discussed 2D single-slice schemes, while enabling a rapid sampling of the third dimension via multislicing.


Conclusion
The unique benefits deriving from fully refocused, multislice, single-scan SPEN sequences were corroborated by phantom tests, as well as by in vivo scans at 3 and 7 T. Low specific absorption rate multislice SPEN variants compatible with human studies were demonstrated. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24711" xmlns="http://purl.org/rss/1.0/"><title>Single shot fast spin echo diffusion imaging with correction for non-linear phase errors using tailored RF pulses</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24711</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Single shot fast spin echo diffusion imaging with correction for non-linear phase errors using tailored RF pulses</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rita G. Nunes, Shaihan J. Malik, Joseph V. Hajnal</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-05T16:19:00.830476-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24711</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24711</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24711</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24711-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The use of tailored RF excitation pulses for prospective correction of non-linear motion-induced phase patterns is shown to enable diffusion-weighted (DW) fast spin echo (FSE) imaging in vivo. Echo-planar imaging (EPI) remains the most used sequence for DW imaging. Despite being highly sensitive to field inhomogeneities, EPI is robust to motion-induced phase shifts. FSE sequences are much less sensitive to field inhomogeneities, but require precise control of the transverse magnetization phase, which is hard to achieve with DW. Real time measurements and correction of phase ramps due to rigid-body motion had been proposed, but performance remained unsatisfactory because of non-linear phase patterns related to pulsatile motion.</p></div></div>
<div class="section" id="mrm24711-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Reproducible non-linear phase components are calibrated using 2D-EPI navigators and tailored RF excitation pulses designed. Real time correction of rigid-body motion was not yet implemented.</p></div></div>
<div class="section" id="mrm24711-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Phase correction was confirmed with full signal DW-FSE images obtained on co-operative subjects. Full diffusion tensor acquisitions were obtained and color-coded maps displaying principal fiber directionality calculated. Results were consistent with corresponding EPI acquisitions except for absence of spatial distortions.</p></div></div>
<div class="section" id="mrm24711-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Combining the proposed method with real time compensation of rigid-body motion has the potential to allow high quality, distortion free diffusion imaging throughout the brain. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
The use of tailored RF excitation pulses for prospective correction of non-linear motion-induced phase patterns is shown to enable diffusion-weighted (DW) fast spin echo (FSE) imaging in vivo. Echo-planar imaging (EPI) remains the most used sequence for DW imaging. Despite being highly sensitive to field inhomogeneities, EPI is robust to motion-induced phase shifts. FSE sequences are much less sensitive to field inhomogeneities, but require precise control of the transverse magnetization phase, which is hard to achieve with DW. Real time measurements and correction of phase ramps due to rigid-body motion had been proposed, but performance remained unsatisfactory because of non-linear phase patterns related to pulsatile motion.


Methods
Reproducible non-linear phase components are calibrated using 2D-EPI navigators and tailored RF excitation pulses designed. Real time correction of rigid-body motion was not yet implemented.


Results
Phase correction was confirmed with full signal DW-FSE images obtained on co-operative subjects. Full diffusion tensor acquisitions were obtained and color-coded maps displaying principal fiber directionality calculated. Results were consistent with corresponding EPI acquisitions except for absence of spatial distortions.


Conclusion
Combining the proposed method with real time compensation of rigid-body motion has the potential to allow high quality, distortion free diffusion imaging throughout the brain. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24697" xmlns="http://purl.org/rss/1.0/"><title>Flip angle mapping with the accelerated 3D look-locker sequence</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24697</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Flip angle mapping with the accelerated 3D look-locker sequence</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Trevor Wade, Charles A. McKenzie, Brian K. Rutt</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-05T16:18:52.581911-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24697</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24697</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24697</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24697-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>A new approach to mapping the flip angle quickly and efficiently in 3D based on the Look-Locker technique is presented.</p></div></div>
<div class="section" id="mrm24697-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>We modified the accelerated 3D Look-Locker <em>T</em><sub>1</sub> measurement technique to allow rapid measurement of flip angle. By removing the inversion pulses and interleaving two radio frequency pulses with different amplitude, it is possible to fit directly for the true flip angle using a reduced number of parameters. This technique, non-inverted Double Angle Look-Locker, allows quick and efficient mapping of the flip angle in 3D.</p></div></div>
<div class="section" id="mrm24697-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>non-inverted Double Angle Look-Locker is validated in vitro against the actual flip angle imaging technique for a range of flip angles and <em>T</em><sub>1</sub> values. Flip angle maps produced with non-inverted Double Angle Look-Locker can be acquired in approximately 1 min, and are accurate to within 10% of the actual flip angle imaging measurement. It is shown to accurately measure the excited slab profile of several different pulses. An application to correcting in vivo DESPOT <em>T</em><sub>1</sub> data is presented.</p></div></div>
<div class="section" id="mrm24697-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The presented technique is a rapid method for mapping flip angles across a 3D volume, capable of producing a flip angle map in approximately 1 min. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
A new approach to mapping the flip angle quickly and efficiently in 3D based on the Look-Locker technique is presented.


Methods
We modified the accelerated 3D Look-Locker T1 measurement technique to allow rapid measurement of flip angle. By removing the inversion pulses and interleaving two radio frequency pulses with different amplitude, it is possible to fit directly for the true flip angle using a reduced number of parameters. This technique, non-inverted Double Angle Look-Locker, allows quick and efficient mapping of the flip angle in 3D.


Results
non-inverted Double Angle Look-Locker is validated in vitro against the actual flip angle imaging technique for a range of flip angles and T1 values. Flip angle maps produced with non-inverted Double Angle Look-Locker can be acquired in approximately 1 min, and are accurate to within 10% of the actual flip angle imaging measurement. It is shown to accurately measure the excited slab profile of several different pulses. An application to correcting in vivo DESPOT T1 data is presented.


Conclusion
The presented technique is a rapid method for mapping flip angles across a 3D volume, capable of producing a flip angle map in approximately 1 min. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24695" xmlns="http://purl.org/rss/1.0/"><title>Respiration based steering for high intensity focused ultrasound liver ablation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24695</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Respiration based steering for high intensity focused ultrasound liver ablation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Andrew B. Holbrook, Pejman Ghanouni, Juan M. Santos, Charles Dumoulin, Yoav Medan, Kim Butts Pauly</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-04T13:06:31.699884-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24695</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24695</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24695</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>Respiratory motion makes hepatic ablation using high intensity focused ultrasound (HIFO) challenging. Previous HIFU liver treatment had required apnea induced during general anesthesia. We describe and test a system that allows treatment of the liver in the presence of breathing motion.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>Mapping a signal from an external respiratory bellow to treatment locations within the liver allows the ultrasound transducer to be steered in real time to the target location. Using a moving phantom, three metrics were used to compare static, steered, and unsteered sonications: the area of sonications once a temperature rise of 15°C was achieved, the energy deposition required to reach that temperature, and the average rate of temperature rise during the first 10 s of sonication. Steered HIFU in vivo ablations of the porcine liver were also performed and compared to breath-hold ablations.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>For the last phantom metric, all groups were found to be statistically significantly different (<em>P</em> ≤ 0.003). However, in the other two metrics, the static and unsteered sonications were not statistically different (<em>P</em> &gt; 0.9999). Steered in vivo HIFU ablations were not statistically significantly different from ablations during breath-holding.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions:</h4><div class="para"><p>A system for performing HIFU steering during ablation of the liver with breathing motion is presented and shown to achieve results equivalent to ablation performed with breath-holding. <b>Magn Reson Med 000:000-000, 2012. © 2012 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>


Purpose:
Respiratory motion makes hepatic ablation using high intensity focused ultrasound (HIFO) challenging. Previous HIFU liver treatment had required apnea induced during general anesthesia. We describe and test a system that allows treatment of the liver in the presence of breathing motion.


Methods:
Mapping a signal from an external respiratory bellow to treatment locations within the liver allows the ultrasound transducer to be steered in real time to the target location. Using a moving phantom, three metrics were used to compare static, steered, and unsteered sonications: the area of sonications once a temperature rise of 15°C was achieved, the energy deposition required to reach that temperature, and the average rate of temperature rise during the first 10 s of sonication. Steered HIFU in vivo ablations of the porcine liver were also performed and compared to breath-hold ablations.


Results:
For the last phantom metric, all groups were found to be statistically significantly different (P ≤ 0.003). However, in the other two metrics, the static and unsteered sonications were not statistically different (P &gt; 0.9999). Steered in vivo HIFU ablations were not statistically significantly different from ablations during breath-holding.


Conclusions:
A system for performing HIFU steering during ablation of the liver with breathing motion is presented and shown to achieve results equivalent to ablation performed with breath-holding. Magn Reson Med 000:000-000, 2012. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24700" xmlns="http://purl.org/rss/1.0/"><title>Acceleration apportionment: A method of improved 2D SENSE acceleration applied to 3D contrast-enhanced MR angiography</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24700</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Acceleration apportionment: A method of improved 2D SENSE acceleration applied to 3D contrast-enhanced MR angiography</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Paul T. Weavers, Eric A. Borisch, Casey P. Johnson, Stephen J. Riederer</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-28T15:59:56.331561-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24700</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24700</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24700</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24700-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>In 2D SENSE-accelerated 3D Cartesian acquisition, the net acceleration factor <em>R</em> is the product of the two individual accelerations, <em>R</em> = <em>R<sub>Y</sub></em> × <em>R<sub>Z</sub></em>. Acceleration Apportionment tailors acceleration parameters (<em>R<sub>Y</sub></em>, <em>R<sub>Z</sub></em>) to improve parallel imaging performance on a patient- and coil-specific basis and is demonstrated in contrast-enhanced MR angiography.</p></div></div>
<div class="section" id="mrm24700-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A performance metric is defined based on coil sensitivity information which identifies the (<em>R<sub>Y</sub></em>, <em>R<sub>Z</sub></em>) pair that optimally trades off image quality with scan time reduction on a patient-specific basis. Acceleration Apportionment is evaluated using retrospective analysis of contrast-enhanced MR angiography studies, and prospective studies in which optimally apportioned parameters are compared with standard acceleration parameters.</p></div></div>
<div class="section" id="mrm24700-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The retrospective studies show strong variability in optimal acceleration parameters between anatomic regions and between patients. Prospective application of apportionment to foot contrast-enhanced MR angiography with an 8-channel receiver array provides a 20% increase in net acceleration with improved contrast-to-noise ratio. Application to 16-channel contrast-enhanced MR angiography of the feet and calves suggests 10% acceleration increase to <em>R</em> &gt; 13 and no contrast-to-noise ratio loss. The specific implementation allows the optimum (<em>R<sub>Y</sub></em>, <em>R<sub>Z</sub></em>) pair to be determined within one minute.</p></div></div>
<div class="section" id="mrm24700-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Optimum 2D SENSE acceleration parameters can be automatically chosen on a per-exam basis to allow improved performance without disrupting the clinical workflow. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
In 2D SENSE-accelerated 3D Cartesian acquisition, the net acceleration factor R is the product of the two individual accelerations, R = RY × RZ. Acceleration Apportionment tailors acceleration parameters (RY, RZ) to improve parallel imaging performance on a patient- and coil-specific basis and is demonstrated in contrast-enhanced MR angiography.


Methods
A performance metric is defined based on coil sensitivity information which identifies the (RY, RZ) pair that optimally trades off image quality with scan time reduction on a patient-specific basis. Acceleration Apportionment is evaluated using retrospective analysis of contrast-enhanced MR angiography studies, and prospective studies in which optimally apportioned parameters are compared with standard acceleration parameters.


Results
The retrospective studies show strong variability in optimal acceleration parameters between anatomic regions and between patients. Prospective application of apportionment to foot contrast-enhanced MR angiography with an 8-channel receiver array provides a 20% increase in net acceleration with improved contrast-to-noise ratio. Application to 16-channel contrast-enhanced MR angiography of the feet and calves suggests 10% acceleration increase to R &gt; 13 and no contrast-to-noise ratio loss. The specific implementation allows the optimum (RY, RZ) pair to be determined within one minute.


Conclusion
Optimum 2D SENSE acceleration parameters can be automatically chosen on a per-exam basis to allow improved performance without disrupting the clinical workflow. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24709" xmlns="http://purl.org/rss/1.0/"><title>High-resolution multishot spiral diffusion tensor imaging with inherent correction of motion-induced phase errors</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24709</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High-resolution multishot spiral diffusion tensor imaging with inherent correction of motion-induced phase errors</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Trong-Kha Truong, Arnaud Guidon</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-28T12:36:20.172605-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24709</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24709</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24709</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24709-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To develop and compare three novel reconstruction methods designed to inherently correct for motion-induced phase errors in multishot spiral diffusion tensor imaging without requiring a variable-density spiral trajectory or a navigator echo.</p></div></div>
<div class="section" id="mrm24709-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>The first method simply averages magnitude images reconstructed with sensitivity encoding from each shot, whereas the second and third methods rely on sensitivity encoding to estimate the motion-induced phase error for each shot and subsequently use either a direct phase subtraction or an iterative conjugate gradient algorithm, respectively, to correct for the resulting artifacts. Numerical simulations and in vivo experiments on healthy volunteers were performed to assess the performance of these methods.</p></div></div>
<div class="section" id="mrm24709-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The first two methods suffer from a low signal-to-noise ratio or from residual artifacts in the reconstructed diffusion-weighted images and fractional anisotropy maps. In contrast, the third method provides high-quality, high-resolution diffusion tensor imaging results, revealing fine anatomical details such as a radial diffusion anisotropy in cortical gray matter.</p></div></div>
<div class="section" id="mrm24709-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The proposed sensitivity encoding + conjugate gradient method can inherently and effectively correct for phase errors, signal loss, and aliasing artifacts caused by both rigid and nonrigid motion in multishot spiral diffusion tensor imaging, without increasing the scan time or reducing the signal-to-noise ratio. <b>Magn Reson Med 000:000–000, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
To develop and compare three novel reconstruction methods designed to inherently correct for motion-induced phase errors in multishot spiral diffusion tensor imaging without requiring a variable-density spiral trajectory or a navigator echo.


Theory and Methods
The first method simply averages magnitude images reconstructed with sensitivity encoding from each shot, whereas the second and third methods rely on sensitivity encoding to estimate the motion-induced phase error for each shot and subsequently use either a direct phase subtraction or an iterative conjugate gradient algorithm, respectively, to correct for the resulting artifacts. Numerical simulations and in vivo experiments on healthy volunteers were performed to assess the performance of these methods.


Results
The first two methods suffer from a low signal-to-noise ratio or from residual artifacts in the reconstructed diffusion-weighted images and fractional anisotropy maps. In contrast, the third method provides high-quality, high-resolution diffusion tensor imaging results, revealing fine anatomical details such as a radial diffusion anisotropy in cortical gray matter.


Conclusion
The proposed sensitivity encoding + conjugate gradient method can inherently and effectively correct for phase errors, signal loss, and aliasing artifacts caused by both rigid and nonrigid motion in multishot spiral diffusion tensor imaging, without increasing the scan time or reducing the signal-to-noise ratio. Magn Reson Med 000:000–000, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24692" xmlns="http://purl.org/rss/1.0/"><title>Renal perfusion imaging with two-dimensional navigator gated arterial spin labeling</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24692</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Renal perfusion imaging with two-dimensional navigator gated arterial spin labeling</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Huan Tan, Ioannis Koktzoglou, Pottumarthi V. Prasad</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-27T13:05:29.230749-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24692</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24692</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24692</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24692-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To develop a navigator technique enabling free-breathing acquisition to afford sufficient signal averaging for quantitative renal perfusion measurement using arterial spin labeling MRI.</p></div></div>
<div class="section" id="mrm24692-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A novel two-dimensional (2D) navigator technique was implemented in concert with flow-sensitive alternating inversion recovery (FAIR) preparation and true fast imaging with steady precession (True-FISP) readout. The navigator images were obtained with a low-resolution fast low angle shot readout at end of each arterial spin labeling acquisition. A retrospective algorithm was developed to automatically detect respiratory motion for selective signal averaging. The 2D navigator-gated FAIR True-FISP sequence was performed in ten healthy volunteers and five patients with chronic kidney disease.</p></div></div>
<div class="section" id="mrm24692-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Excellent image quality and comparable cortical perfusion rates (healthy: 276 ± 28 mL/100 g/min, patients: 155 ± 25 mL/100 g/min) to literature values were obtained. An average of 3-fold signal-to-noise ratio improvement was obtained in the 2D navigator-gated approach compared with the breath-hold acquisition in healthy volunteers. Good image quality was achieved in patients while the results from breath-hold acquisition were unusable. The quantitative perfusion rates were significantly lower in chronic kidney disease patients compared with the healthy volunteers.</p></div></div>
<div class="section" id="mrm24692-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>2D navigator-gated free breathing arterial spin labeling is feasible and is a noninvasive method to evaluate renal perfusion both in healthy subjects and those with chronic kidney disease. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To develop a navigator technique enabling free-breathing acquisition to afford sufficient signal averaging for quantitative renal perfusion measurement using arterial spin labeling MRI.


Methods
A novel two-dimensional (2D) navigator technique was implemented in concert with flow-sensitive alternating inversion recovery (FAIR) preparation and true fast imaging with steady precession (True-FISP) readout. The navigator images were obtained with a low-resolution fast low angle shot readout at end of each arterial spin labeling acquisition. A retrospective algorithm was developed to automatically detect respiratory motion for selective signal averaging. The 2D navigator-gated FAIR True-FISP sequence was performed in ten healthy volunteers and five patients with chronic kidney disease.


Results
Excellent image quality and comparable cortical perfusion rates (healthy: 276 ± 28 mL/100 g/min, patients: 155 ± 25 mL/100 g/min) to literature values were obtained. An average of 3-fold signal-to-noise ratio improvement was obtained in the 2D navigator-gated approach compared with the breath-hold acquisition in healthy volunteers. Good image quality was achieved in patients while the results from breath-hold acquisition were unusable. The quantitative perfusion rates were significantly lower in chronic kidney disease patients compared with the healthy volunteers.


Conclusion
2D navigator-gated free breathing arterial spin labeling is feasible and is a noninvasive method to evaluate renal perfusion both in healthy subjects and those with chronic kidney disease. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24691" xmlns="http://purl.org/rss/1.0/"><title>A noninvasive tumor oxygenation imaging strategy using magnetic resonance imaging of endogenous blood and tissue water</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24691</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A noninvasive tumor oxygenation imaging strategy using magnetic resonance imaging of endogenous blood and tissue water</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhongwei Zhang, Rami R. Hallac, Peter Peschke, Ralph P. Mason</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-27T13:05:20.259356-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24691</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24691</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24691</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24691-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To present a novel imaging strategy for noninvasive measurement of tumor oxygenation using MR imaging of endogenous blood and tissue water.</p></div></div>
<div class="section" id="mrm24691-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>The proposed approach for oxygen partial pressure (pO<sub>2</sub>) estimation is based on intravoxel incoherent motion diffusion MRI and the dependence of the blood <em>R</em><sub>2</sub> relaxation rate on the inter-echo spacing measured using a multiple spin-echo Carr-Purcell-Meiboom-Gill sequence and weak-field diffusion model. The accuracy of the approach was validated by comparison with <sup>19</sup>F MRI oximetry.</p></div></div>
<div class="section" id="mrm24691-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The results in eight rats at 4.7 T showed that tumors have longer <em>T</em><sub>1</sub> (1980 ± 186 ms) and <em>T</em><sub>2</sub> (59 ± 9 ms) relaxation times, heterogeneous blood volume fraction (0.23 ± 0.1), oxygen saturation level (<em>Y</em>) (0.53 ± 0.12), and pO<sub>2</sub> (36 ± 15 mmHg) distributions compared with normal muscle (<em>T</em><sub>1</sub> 1480 ± 86 ms, <em>T</em><sub>2</sub> 29 ± 2 ms, blood volume fraction 0.22 ± 0.03, <em>Y</em> 0.49 ± 0.06, and pO<sub>2</sub> 39 ± 5 mmHg). pO<sub>2</sub> estimates based on the novel <sup>1</sup>H approach were essentially identical with <sup>19</sup>F observations.</p></div></div>
<div class="section" id="mrm24691-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The study indicates that noninvasive measurement of tumor pO<sub>2</sub> using <sup>1</sup>H MRI derived multiparametric maps is feasible and could become a valuable tool to evaluate tumor hypoxia.</p></div></div>
]]></content:encoded><description>

Purpose
To present a novel imaging strategy for noninvasive measurement of tumor oxygenation using MR imaging of endogenous blood and tissue water.


Theory and Methods
The proposed approach for oxygen partial pressure (pO2) estimation is based on intravoxel incoherent motion diffusion MRI and the dependence of the blood R2 relaxation rate on the inter-echo spacing measured using a multiple spin-echo Carr-Purcell-Meiboom-Gill sequence and weak-field diffusion model. The accuracy of the approach was validated by comparison with 19F MRI oximetry.


Results
The results in eight rats at 4.7 T showed that tumors have longer T1 (1980 ± 186 ms) and T2 (59 ± 9 ms) relaxation times, heterogeneous blood volume fraction (0.23 ± 0.1), oxygen saturation level (Y) (0.53 ± 0.12), and pO2 (36 ± 15 mmHg) distributions compared with normal muscle (T1 1480 ± 86 ms, T2 29 ± 2 ms, blood volume fraction 0.22 ± 0.03, Y 0.49 ± 0.06, and pO2 39 ± 5 mmHg). pO2 estimates based on the novel 1H approach were essentially identical with 19F observations.


Conclusion
The study indicates that noninvasive measurement of tumor pO2 using 1H MRI derived multiparametric maps is feasible and could become a valuable tool to evaluate tumor hypoxia.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24687" xmlns="http://purl.org/rss/1.0/"><title>Fe(III) distribution varies substantially within and between atherosclerotic plaques</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24687</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Fe(III) distribution varies substantially within and between atherosclerotic plaques</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">H. Gustafsson, M. Hallbeck, M. Norell, M. Lindgren, M. Engström, A. Rosén, H. Zachrisson</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-27T13:05:05.435339-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24687</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24687</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24687</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24687-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Vulnerable atherosclerotic plaques are structurally weak and prone to rupture, presumably due to local oxidative stress. Redox active iron is linked to oxidative stress and the aim of this study was to investigate the distribution of Fe(III) in carotid plaques and its relation to vulnerability for rupture.</p></div></div>
<div class="section" id="mrm24687-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Atherosclerotic plaques from 10 patients (three asymptomatic and seven symptomatic) were investigated. Plaque vulnerability was classified using ultrasound and immunohistochemistry and correlated to Fe(III) measured by electron paramagnetic resonance spectroscopy.</p></div></div>
<div class="section" id="mrm24687-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Large intra-plaque Fe(III) variations were found. Plaques from symptomatic patients had a higher Fe(III) concentration as compared with asymptomatic plaques (0.36 ± 0.21 vs. 0.06 ± 0.04 nmol Fe(III)/mg tissue, <em>P</em> &lt; 0.05, in sections adjoining narrowest part of the plaques). All but one plaque from symptomatic patients showed signs of cap rupture. No plaque from asymptomatic patients showed signs of cap rupture. There was a significant increase in cap macrophages in plaques from symptomatic patients compared with asymptomatic patients (31 ± 11% vs. 2.3 ± 2.3%, <em>P</em> &lt; 0.01).</p></div></div>
<div class="section" id="mrm24687-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Fe(III) distribution varies substantially within atherosclerotic plaques. Plaques from symptomatic patients had significantly higher concentrations of Fe(III), signs of cap rupture and increased cap macrophage activity. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Vulnerable atherosclerotic plaques are structurally weak and prone to rupture, presumably due to local oxidative stress. Redox active iron is linked to oxidative stress and the aim of this study was to investigate the distribution of Fe(III) in carotid plaques and its relation to vulnerability for rupture.


Methods
Atherosclerotic plaques from 10 patients (three asymptomatic and seven symptomatic) were investigated. Plaque vulnerability was classified using ultrasound and immunohistochemistry and correlated to Fe(III) measured by electron paramagnetic resonance spectroscopy.


Results
Large intra-plaque Fe(III) variations were found. Plaques from symptomatic patients had a higher Fe(III) concentration as compared with asymptomatic plaques (0.36 ± 0.21 vs. 0.06 ± 0.04 nmol Fe(III)/mg tissue, P &lt; 0.05, in sections adjoining narrowest part of the plaques). All but one plaque from symptomatic patients showed signs of cap rupture. No plaque from asymptomatic patients showed signs of cap rupture. There was a significant increase in cap macrophages in plaques from symptomatic patients compared with asymptomatic patients (31 ± 11% vs. 2.3 ± 2.3%, P &lt; 0.01).


Conclusion
Fe(III) distribution varies substantially within atherosclerotic plaques. Plaques from symptomatic patients had significantly higher concentrations of Fe(III), signs of cap rupture and increased cap macrophage activity. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24656" xmlns="http://purl.org/rss/1.0/"><title>Functional MRI in human subjects with gradient-echo and spin-echo EPI at 9.4 T</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24656</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Functional MRI in human subjects with gradient-echo and spin-echo EPI at 9.4 T</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Juliane Budde, G. Shajan, Maxim Zaitsev, Klaus Scheffler, Rolf Pohmann</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-27T13:04:48.878807-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24656</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24656</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24656</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24656-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The increased signal-to-noise ratio and blood oxygen level dependent signal at ultra-high field can only help to boost the resolution in functional MRI studies if the spatial specificity of the activation signal is improved. At a field strength of 9.4 T, both gradient-echo and spin-echo based echo-planar imaging were implemented and applied to investigate the specificity of human functional MRI. A finger tapping paradigm was used to acquire functional MRI data with scan parameters similar to standard neuroscientific applications.</p></div></div>
<div class="section" id="mrm24656-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Spatial resolution, echo, and readout times were varied to determine their influence on the distribution of the blood oxygen level dependent signal. High-resolution co-localized images were used to classify the signal according to its origin in veins or tissue.</p></div></div>
<div class="section" id="mrm24656-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>High-quality activation maps were obtained with both sequences. Signal contributions from tissue were found to be smaller or slightly larger than from veins. Gradient-echo echo-planar imaging yielded lower ratios of micro-/macro-vascular signals of around 0.6 than spin-echo based functional MRI, where this ratio varied between 0.75 and 1.02, with higher values for larger echo and shorter readout time.</p></div></div>
<div class="section" id="mrm24656-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>This study demonstrates the feasibility of human functional MRI at 9.4 T with high spatial specificity. Although venous contributions could not be entirely suppressed, venous effects in spin-echo echo-planar imaging are significantly reduced compared with gradient-echo echo-planar imaging. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The increased signal-to-noise ratio and blood oxygen level dependent signal at ultra-high field can only help to boost the resolution in functional MRI studies if the spatial specificity of the activation signal is improved. At a field strength of 9.4 T, both gradient-echo and spin-echo based echo-planar imaging were implemented and applied to investigate the specificity of human functional MRI. A finger tapping paradigm was used to acquire functional MRI data with scan parameters similar to standard neuroscientific applications.


Methods
Spatial resolution, echo, and readout times were varied to determine their influence on the distribution of the blood oxygen level dependent signal. High-resolution co-localized images were used to classify the signal according to its origin in veins or tissue.


Results
High-quality activation maps were obtained with both sequences. Signal contributions from tissue were found to be smaller or slightly larger than from veins. Gradient-echo echo-planar imaging yielded lower ratios of micro-/macro-vascular signals of around 0.6 than spin-echo based functional MRI, where this ratio varied between 0.75 and 1.02, with higher values for larger echo and shorter readout time.


Conclusion
This study demonstrates the feasibility of human functional MRI at 9.4 T with high spatial specificity. Although venous contributions could not be entirely suppressed, venous effects in spin-echo echo-planar imaging are significantly reduced compared with gradient-echo echo-planar imaging. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24632" xmlns="http://purl.org/rss/1.0/"><title>In vivo investigation of restricted diffusion in the human brain with optimized oscillating diffusion gradient encoding</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24632</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">In vivo investigation of restricted diffusion in the human brain with optimized oscillating diffusion gradient encoding</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Anh T. Van, Samantha J. Holdsworth, Roland Bammer</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-27T13:04:44.186773-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24632</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24632</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24632</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24632-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Previous studies in phantoms and animals using animal MR systems have shown promising results in using oscillating gradient spin echo (OGSE) diffusion acquisition to depict microstructure information. The OGSE approach has also been shown to be a sensitive biomarker of tumor treatment response and white matter-related diseases. Translating these studies to a human MR scanner faces multiple challenges due to the much weaker gradient system. The goals of this study are to optimize the OGSE acquisition for a human MR system and investigate its applicability in the in vivo human brain.</p></div></div>
<div class="section" id="mrm24632-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>An analytical analysis of the OGSE modulation spectrum was provided. Based on this analysis and thorough simulation experiments, the OGSE acquisition was optimized in terms of diffusion waveform shape, waveform timing, and sequence timing—to achieve higher diffusion sensitivity and better sampling of the diffusion spectrum.</p></div></div>
<div class="section" id="mrm24632-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The trapezoid-cosine waveform was found to be the optimal OGSE waveform. At the three employed peak encoding frequencies of 18 Hz, 44 Hz, and 63 Hz, the waveform polarity for the least blurry sampling of the diffusion spectrum was 90+/180−, 90+/180+, and 90+/180+, respectively. For the highest diffusion-to-noise ratio at 63 Hz, the <em>b</em>-value was 200 s/mm<sup>2</sup> and the echo time was 116 ms. Using the optimized sequence, a frequency dependence of the measured apparent diffusion coefficients was observed in white matter-dominant regions such as the corpus callosum.</p></div></div>
<div class="section" id="mrm24632-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The obtained results demonstrate, for the first time, the potential of using an OGSE acquisition for investigating microstructure information on a human MR system. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Previous studies in phantoms and animals using animal MR systems have shown promising results in using oscillating gradient spin echo (OGSE) diffusion acquisition to depict microstructure information. The OGSE approach has also been shown to be a sensitive biomarker of tumor treatment response and white matter-related diseases. Translating these studies to a human MR scanner faces multiple challenges due to the much weaker gradient system. The goals of this study are to optimize the OGSE acquisition for a human MR system and investigate its applicability in the in vivo human brain.


Methods
An analytical analysis of the OGSE modulation spectrum was provided. Based on this analysis and thorough simulation experiments, the OGSE acquisition was optimized in terms of diffusion waveform shape, waveform timing, and sequence timing—to achieve higher diffusion sensitivity and better sampling of the diffusion spectrum.


Results
The trapezoid-cosine waveform was found to be the optimal OGSE waveform. At the three employed peak encoding frequencies of 18 Hz, 44 Hz, and 63 Hz, the waveform polarity for the least blurry sampling of the diffusion spectrum was 90+/180−, 90+/180+, and 90+/180+, respectively. For the highest diffusion-to-noise ratio at 63 Hz, the b-value was 200 s/mm2 and the echo time was 116 ms. Using the optimized sequence, a frequency dependence of the measured apparent diffusion coefficients was observed in white matter-dominant regions such as the corpus callosum.


Conclusion
The obtained results demonstrate, for the first time, the potential of using an OGSE acquisition for investigating microstructure information on a human MR system. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24645" xmlns="http://purl.org/rss/1.0/"><title>Reproduction of motion artifacts for performance analysis of prospective motion correction in MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24645</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Reproduction of motion artifacts for performance analysis of prospective motion correction in MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Michael Herbst, Julian Maclaren, Cris Lovell-Smith, Rebecca Sostheim, Karl Egger, Andreas Harloff, Jan Korvink, Juergen Hennig, Maxim Zaitsev</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T15:53:50.119142-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24645</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24645</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24645</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>Despite numerous publications describing the ability of prospective motion correction to improve image quality in magnetic resonance imaging of the brain, a reliable approach to assess this improvement is still missing. A method that accurately reproduces motion artifacts correctable with prospective motion correction is developed, and enables the quantification of the improvements achieved.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>A software interface was developed to simulate rigid body motion by changing the scanning coordinate system relative to the object. Thus, tracking data recorded during a patient scan can be used to reproduce the prevented motion artifacts on a volunteer or a phantom. The influence of physiological motion on image quality was investigated by filtering these data. Finally, the method was used to reproduce and quantify the motion artifacts prevented in a patient scan.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>The accuracy of the method was tested in phantom experiments and in vivo. The calculated quality factor, as well as a visual inspection of the reproduced artifacts shows a good correspondence to the original.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>Precise reproduction of motion artifacts assists qualification of prospective motion correction strategies. The presented method provides an important tool to investigate the effects of rigid body motion on a wide range of sequences, and to quantify the improvement in image quality through prospective motion correction. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
Despite numerous publications describing the ability of prospective motion correction to improve image quality in magnetic resonance imaging of the brain, a reliable approach to assess this improvement is still missing. A method that accurately reproduces motion artifacts correctable with prospective motion correction is developed, and enables the quantification of the improvements achieved.


Methods:
A software interface was developed to simulate rigid body motion by changing the scanning coordinate system relative to the object. Thus, tracking data recorded during a patient scan can be used to reproduce the prevented motion artifacts on a volunteer or a phantom. The influence of physiological motion on image quality was investigated by filtering these data. Finally, the method was used to reproduce and quantify the motion artifacts prevented in a patient scan.


Results:
The accuracy of the method was tested in phantom experiments and in vivo. The calculated quality factor, as well as a visual inspection of the reproduced artifacts shows a good correspondence to the original.


Conclusion:
Precise reproduction of motion artifacts assists qualification of prospective motion correction strategies. The presented method provides an important tool to investigate the effects of rigid body motion on a wide range of sequences, and to quantify the improvement in image quality through prospective motion correction. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24678" xmlns="http://purl.org/rss/1.0/"><title>Design, manufacture, and analysis of customized phantoms for enhanced quality control in small animal MRI systems</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24678</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Design, manufacture, and analysis of customized phantoms for enhanced quality control in small animal MRI systems</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Eriko Yoshimaru, John Totenhagen, Gene E. Alexander, Theodore P. Trouard</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T15:26:24.934934-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24678</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24678</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24678</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24678-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Magnetic resonance imaging (MRI) is widely used in human brain research to evaluate the effects of healthy aging and development, as well as neurological disorders. Although standardized methods for quality assurance of human MRI instruments have been established, such approaches have typically not been translated to small animal imaging. We present a method for the generation and analysis of customized phantoms for small animal MRI systems that allows rapid and accurate system stability monitoring.</p></div></div>
<div class="section" id="mrm24678-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Computer-aided design software was used to produce a customized phantom using a rapid prototyping printer. Automated registration algorithms were used on three-dimensional images of the phantom to allow system stability to be easily monitored over time.</p></div></div>
<div class="section" id="mrm24678-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The design of the custom phantom allowed reliable placement relative to the imaging coil. Automated registration showed superior ability to detect gradient changes reflected in the images than with manual measurements. Registering images acquired over time allowed monitoring of gradient drifts of less than one percent.</p></div></div>
<div class="section" id="mrm24678-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>A low cost, MRI compatible phantom was successfully designed using computer-aided design software and a three-dimensional printer. Registering phantom images acquired over time allows monitoring of gradient stability of the MRI system. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Magnetic resonance imaging (MRI) is widely used in human brain research to evaluate the effects of healthy aging and development, as well as neurological disorders. Although standardized methods for quality assurance of human MRI instruments have been established, such approaches have typically not been translated to small animal imaging. We present a method for the generation and analysis of customized phantoms for small animal MRI systems that allows rapid and accurate system stability monitoring.


Methods
Computer-aided design software was used to produce a customized phantom using a rapid prototyping printer. Automated registration algorithms were used on three-dimensional images of the phantom to allow system stability to be easily monitored over time.


Results
The design of the custom phantom allowed reliable placement relative to the imaging coil. Automated registration showed superior ability to detect gradient changes reflected in the images than with manual measurements. Registering images acquired over time allowed monitoring of gradient drifts of less than one percent.


Conclusion
A low cost, MRI compatible phantom was successfully designed using computer-aided design software and a three-dimensional printer. Registering phantom images acquired over time allows monitoring of gradient stability of the MRI system. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24624" xmlns="http://purl.org/rss/1.0/"><title>Diffusion-weighted imaging for evaluation of uterine arterial embolization of fibroids</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24624</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Diffusion-weighted imaging for evaluation of uterine arterial embolization of fibroids</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Nathalie Faye, Olivier Pellerin, Rokhaya Thiam, Foucauld Chammings, Marie Brisa, Enio Marques, Charles A. Cuénod, Marc Sapoval, Laure S. Fournier</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T15:26:09.098484-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24624</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24624</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24624</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24624-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To determine whether diffusion-weighted imaging (DWI) characteristics could predict the effectiveness of uterine arterial embolization in treatment of fibroids.</p></div></div>
<div class="section" id="mrm24624-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>This retrospective study included 17 women (27 fibroids) who underwent uterine arterial embolization for fibroids. MR imaging (1.5 T) was performed before, 1 week and 6 months after uterine arterial embolization. The volume, T2 signal, T1 signal, enhancement after contrast media injection, DWI signal (<em>b</em> = 500 s/mm<sup>2</sup>) and apparent diffusion coefficient (ADC) were assessed for fibroids.</p></div></div>
<div class="section" id="mrm24624-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>DWI signal or ADC, whether before or 1 week after the procedure, did not show a statistical relationship to success of uterine arterial embolization. On the 1-week follow-up, 22% of fibroids enhanced vs. 85% on baseline, <em>P</em>  &lt;  0.0001 and DW signal intensity increased. ADC values in fibroids decreased between baseline and 1-week (1.61 vs. 1.53 × 10<sup>−3</sup> mm<sup>2</sup>/s, <em>P</em> = 0.13). On 6-months, ADC continued to decrease compared with baseline (1.27 × 10<sup>−3</sup> mm<sup>2</sup>/s, <em>P</em> = 0.002), but with a lower signal on DWI. No changes were observed in myometrium ADC at any time point.</p></div></div>
<div class="section" id="mrm24624-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Our study demonstrated that DWI and ADC reflected early and delayed changes in fibroids after embolization; however, we were not able to demonstrate a statistically significant relationship with outcome. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To determine whether diffusion-weighted imaging (DWI) characteristics could predict the effectiveness of uterine arterial embolization in treatment of fibroids.


Methods
This retrospective study included 17 women (27 fibroids) who underwent uterine arterial embolization for fibroids. MR imaging (1.5 T) was performed before, 1 week and 6 months after uterine arterial embolization. The volume, T2 signal, T1 signal, enhancement after contrast media injection, DWI signal (b = 500 s/mm2) and apparent diffusion coefficient (ADC) were assessed for fibroids.


Results
DWI signal or ADC, whether before or 1 week after the procedure, did not show a statistical relationship to success of uterine arterial embolization. On the 1-week follow-up, 22% of fibroids enhanced vs. 85% on baseline, P  &lt;  0.0001 and DW signal intensity increased. ADC values in fibroids decreased between baseline and 1-week (1.61 vs. 1.53 × 10−3 mm2/s, P = 0.13). On 6-months, ADC continued to decrease compared with baseline (1.27 × 10−3 mm2/s, P = 0.002), but with a lower signal on DWI. No changes were observed in myometrium ADC at any time point.


Conclusion
Our study demonstrated that DWI and ADC reflected early and delayed changes in fibroids after embolization; however, we were not able to demonstrate a statistically significant relationship with outcome. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24643" xmlns="http://purl.org/rss/1.0/"><title>Correction of gradient-induced phase errors in radial MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24643</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Correction of gradient-induced phase errors in radial MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Amir Moussavi, Markus Untenberger, Martin Uecker, Jens Frahm</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T15:26:01.845298-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24643</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24643</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24643</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24643-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To correct gradient-induced phase errors in radial MRI.</p></div></div>
<div class="section" id="mrm24643-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Gradient-induced eddy currents affect the MRI data acquisition by gradient delays and phase errors that may lead to severe image artifacts for non-Cartesian imaging scenarios such as radial trajectories. While gradient delays are dealt with by respective shifts of the acquisition window during radial image acquisition, this work introduces a simple method for quantifying and correcting phase errors from the actual data prior to image reconstruction. For a given gradient system, the approach yields a specific phase error per gradient that can be used for correcting the raw data.</p></div></div>
<div class="section" id="mrm24643-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Phantom studies at 9.4 T demonstrated marked improvements in radial image quality. It could be shown that the phase correction is not compromised by data undersampling. Moreover, the selective correction of gradient-induced phase errors retained the phase information caused by different concentrations of a paramagnetic contrast agent.</p></div></div>
<div class="section" id="mrm24643-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The proposed method does not require additional reference measurements and separately corrects for phase errors induced by eddy currents, while retaining the residual phase of the object which may carry physiologic information. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To correct gradient-induced phase errors in radial MRI.


Methods
Gradient-induced eddy currents affect the MRI data acquisition by gradient delays and phase errors that may lead to severe image artifacts for non-Cartesian imaging scenarios such as radial trajectories. While gradient delays are dealt with by respective shifts of the acquisition window during radial image acquisition, this work introduces a simple method for quantifying and correcting phase errors from the actual data prior to image reconstruction. For a given gradient system, the approach yields a specific phase error per gradient that can be used for correcting the raw data.


Results
Phantom studies at 9.4 T demonstrated marked improvements in radial image quality. It could be shown that the phase correction is not compromised by data undersampling. Moreover, the selective correction of gradient-induced phase errors retained the phase information caused by different concentrations of a paramagnetic contrast agent.


Conclusion
The proposed method does not require additional reference measurements and separately corrects for phase errors induced by eddy currents, while retaining the residual phase of the object which may carry physiologic information. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24675" xmlns="http://purl.org/rss/1.0/"><title>Spiral trajectory design: A flexible numerical algorithm and base analytical equations</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24675</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Spiral trajectory design: A flexible numerical algorithm and base analytical equations</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">James G. Pipe, Nicholas R. Zwart</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T15:23:33.185979-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24675</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24675</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24675</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24675-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Spiral-based trajectories for magnetic resonance imaging can be advantageous, but are often cumbersome to design or create. This work presents a flexible numerical algorithm for designing trajectories based on explicit definition of radial undersampling, and also gives several analytical expressions for charactering the base (critically sampled) class of these trajectories.</p></div></div>
<div class="section" id="mrm24675-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>Expressions for the gradient waveform, based on slew and amplitude limits, are developed such that a desired pitch in the spiral k-space trajectory is followed. The source code for this algorithm, written in C, is publicly available. Analytical expressions approximating the spiral trajectory (ignoring the radial component) are given to characterize measurement time, gradient heating, maximum gradient amplitude, and off-resonance phase for slew-limited and gradient amplitude-limited cases. Several numerically calculated trajectories are illustrated, and base Archimedean spirals are compared with analytically obtained results.</p></div></div>
<div class="section" id="mrm24675-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Several different waveforms illustrate that the desired slew and amplitude limits are reached, as are the desired undersampling patterns, using the numerical method. For base Archimedean spirals, the results of the numerical and analytical approaches are in good agreement.</p></div></div>
<div class="section" id="mrm24675-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>A versatile numerical algorithm was developed, and was written in publicly available code. Approximate analytical formulas are given that help characterize spiral trajectories. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Spiral-based trajectories for magnetic resonance imaging can be advantageous, but are often cumbersome to design or create. This work presents a flexible numerical algorithm for designing trajectories based on explicit definition of radial undersampling, and also gives several analytical expressions for charactering the base (critically sampled) class of these trajectories.


Theory and Methods
Expressions for the gradient waveform, based on slew and amplitude limits, are developed such that a desired pitch in the spiral k-space trajectory is followed. The source code for this algorithm, written in C, is publicly available. Analytical expressions approximating the spiral trajectory (ignoring the radial component) are given to characterize measurement time, gradient heating, maximum gradient amplitude, and off-resonance phase for slew-limited and gradient amplitude-limited cases. Several numerically calculated trajectories are illustrated, and base Archimedean spirals are compared with analytically obtained results.


Results
Several different waveforms illustrate that the desired slew and amplitude limits are reached, as are the desired undersampling patterns, using the numerical method. For base Archimedean spirals, the results of the numerical and analytical approaches are in good agreement.


Conclusion
A versatile numerical algorithm was developed, and was written in publicly available code. Approximate analytical formulas are given that help characterize spiral trajectories. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24681" xmlns="http://purl.org/rss/1.0/"><title>Fast accurate MR thermometry using phase referenced asymmetric spin-echo EPI at high field</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24681</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Fast accurate MR thermometry using phase referenced asymmetric spin-echo EPI at high field</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Markus N. Streicher, Andreas Schäfer, Dimo Ivanov, Dirk K. Müller, Alexis Amadon, Enrico Reimer, Laurentius Huber, Bibek Dhital, Debra Rivera, Carsten Kögler, Robert Trampel, André Pampel, Robert Turner</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T15:20:37.486955-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24681</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24681</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24681</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24681-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>A novel highly accurate method for MR thermometry, effective at high field, is introduced and validated, which corrects for slow and fast field fluctuations by means of reference images.</p></div></div>
<div class="section" id="mrm24681-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>An asymmetric spin-echo echo planar imaging sequence was made frequency-selective to water or a reference substance by controlling the slice-select gradient polarity and the duration of the excitation and refocusing radiofrequency pulses. Images were acquired pairwise, and the temperature-sensitive water images were corrected for field fluctuations using the reference images. In a phantom radiofrequency heating experiment, dissolved dimethyl sulfoxide was used as a reference substance. Temperature stability was tested in vivo on the human brain, referenced using subcutaneous scalp fat. Water and fat phase images were acquired only 50 ms apart. Bloch simulations validated the frequency selection accuracy.</p></div></div>
<div class="section" id="mrm24681-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Asymmetric spin-echo imaging using a simple frequency selection method provides highly accurate referenced MR thermometry in phantoms and in vivo at 7 T. Effects of field fluctuations caused by field drift, breathing, and heart beat were corrected. The technique is highly robust against <em>B</em><sub>1</sub> inhomogeneities.</p></div></div>
<div class="section" id="mrm24681-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Frequency selection using gradient-reversal can enable fast accurate referenced in vivo MR thermometry, assisting thermal characterization of radiofrequency coils and possibly in vivo SAR monitoring. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
A novel highly accurate method for MR thermometry, effective at high field, is introduced and validated, which corrects for slow and fast field fluctuations by means of reference images.


Methods
An asymmetric spin-echo echo planar imaging sequence was made frequency-selective to water or a reference substance by controlling the slice-select gradient polarity and the duration of the excitation and refocusing radiofrequency pulses. Images were acquired pairwise, and the temperature-sensitive water images were corrected for field fluctuations using the reference images. In a phantom radiofrequency heating experiment, dissolved dimethyl sulfoxide was used as a reference substance. Temperature stability was tested in vivo on the human brain, referenced using subcutaneous scalp fat. Water and fat phase images were acquired only 50 ms apart. Bloch simulations validated the frequency selection accuracy.


Results
Asymmetric spin-echo imaging using a simple frequency selection method provides highly accurate referenced MR thermometry in phantoms and in vivo at 7 T. Effects of field fluctuations caused by field drift, breathing, and heart beat were corrected. The technique is highly robust against B1 inhomogeneities.


Conclusion
Frequency selection using gradient-reversal can enable fast accurate referenced in vivo MR thermometry, assisting thermal characterization of radiofrequency coils and possibly in vivo SAR monitoring. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24690" xmlns="http://purl.org/rss/1.0/"><title>Whole-body and local RF absorption in human models as a function of anatomy and position within 1.5T MR body coil</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24690</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Whole-body and local RF absorption in human models as a function of anatomy and position within 1.5T MR body coil</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Manuel Murbach, Esra Neufeld, Wolfgang Kainz, Klaas P. Pruessmann, Niels Kuster</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T15:18:49.548297-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24690</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24690</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24690</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24690-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Radiofrequency energy deposition in magnetic resonance imaging must be limited to prevent excessive heating of the patient. Correlations of radiofrequency absorption with large-scale anatomical features (e.g., height) are investigated in this article.</p></div></div>
<div class="section" id="mrm24690-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>The specific absorption rate (SAR), as the pivotal parameter for quantifying absorbed radiofrequency, increases with the radial dimension of the patient and therefore with the large-scale anatomical properties. The absorbed energy in six human models has been modeled in different Z-positions (head to knees) within a 1.5T bodycoil.</p></div></div>
<div class="section" id="mrm24690-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>For a fixed 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24690/asset/equation/mrm24690-math-0001.gif?v=1&amp;t=hh1lk4bk&amp;s=310a417b8f5d703308fe8537b1f6a23071f90718" class="inlineGraphic"/> incident field, the whole-body SAR can be up to 2.5 times higher (local SAR up to seven times) in obese adult models compared to children. If the exposure is normalized to 4 W/kg whole-body SAR, the local SAR can well-exceed the limits for local transmit coils and shows intersubject variations of up to a factor of three.</p></div></div>
<div class="section" id="mrm24690-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>The correlations between anatomy and induced local SAR are weak for normalized exposure, but strong for a fixed 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24690/asset/equation/mrm24690-math-0002.gif?v=1&amp;t=hh1lk4bm&amp;s=37a29eeb591a11218b70bf2676f9527e06c7aa92" class="inlineGraphic"/> field, suggesting that anatomical properties could be used for fast SAR predictions. This study demonstrates that a representative virtual human population is indispensable for the investigation of local SAR levels. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Radiofrequency energy deposition in magnetic resonance imaging must be limited to prevent excessive heating of the patient. Correlations of radiofrequency absorption with large-scale anatomical features (e.g., height) are investigated in this article.


Theory and Methods
The specific absorption rate (SAR), as the pivotal parameter for quantifying absorbed radiofrequency, increases with the radial dimension of the patient and therefore with the large-scale anatomical properties. The absorbed energy in six human models has been modeled in different Z-positions (head to knees) within a 1.5T bodycoil.


Results
For a fixed 
B1+ incident field, the whole-body SAR can be up to 2.5 times higher (local SAR up to seven times) in obese adult models compared to children. If the exposure is normalized to 4 W/kg whole-body SAR, the local SAR can well-exceed the limits for local transmit coils and shows intersubject variations of up to a factor of three.


Conclusions
The correlations between anatomy and induced local SAR are weak for normalized exposure, but strong for a fixed 
B1+ field, suggesting that anatomical properties could be used for fast SAR predictions. This study demonstrates that a representative virtual human population is indispensable for the investigation of local SAR levels. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24684" xmlns="http://purl.org/rss/1.0/"><title>Quick water-selective excitation of fast relaxing tissues with 3D UTE sequences</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24684</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Quick water-selective excitation of fast relaxing tissues with 3D UTE sequences</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Fabian Springer, Günter Steidle, Petros Martirosian, Ulrich Grosse, Roland Syha, Christoph Schabel, Claus D. Claussen, Fritz Schick</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T15:17:22.827347-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24684</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24684</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24684</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24684-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The aim of this study was to implement a time effective 1-1 double pulse water-selective excitation (WE) into a three-dimensional ultrashort echo time (UTE) sequence (WE-UTE) for visualization of short-<em>T</em><sub>2</sub> tissues with positive contrast and sufficient suppression of surrounding fat.</p></div></div>
<div class="section" id="mrm24684-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>First, an analytical description of magnetization components in the steady state applying WE-UTE was derived and results were compared with numerical simulations based on Bloch's equations. Parameters were optimized for best positive contrast between short-<em>T</em><sub>2</sub> tissues and fat under consideration of variable relaxation properties over a broad range. Maximal signal yield and signal efficiency of on-resonant protons were compared with UTE sequences with and without off-resonance fat saturation (FatSat). WE-UTE was exemplarily applied for in-vivo musculoskeletal imaging on a 3T whole-body MR unit.</p></div></div>
<div class="section" id="mrm24684-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Steady state magnetization of WE-UTE could be described analytically and showed excellent accordance with numerical simulations. Even for tissues with <em>T</em><sub>2</sub> = 1 ms WE-UTE resulted in 79% of maximal signal yield of UTE without FatSat and was more efficient regarding signal yield if compared with UTE with FatSat. Using WE-UTE in-vivo tendons and ligaments could be well delineated with positive contrast to surrounding fat.</p></div></div>
<div class="section" id="mrm24684-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>WE-UTE provides a quick method for visualizing short-<em>T</em><sub>2</sub> tissues with positive contrast. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The aim of this study was to implement a time effective 1-1 double pulse water-selective excitation (WE) into a three-dimensional ultrashort echo time (UTE) sequence (WE-UTE) for visualization of short-T2 tissues with positive contrast and sufficient suppression of surrounding fat.


Methods
First, an analytical description of magnetization components in the steady state applying WE-UTE was derived and results were compared with numerical simulations based on Bloch's equations. Parameters were optimized for best positive contrast between short-T2 tissues and fat under consideration of variable relaxation properties over a broad range. Maximal signal yield and signal efficiency of on-resonant protons were compared with UTE sequences with and without off-resonance fat saturation (FatSat). WE-UTE was exemplarily applied for in-vivo musculoskeletal imaging on a 3T whole-body MR unit.


Results
Steady state magnetization of WE-UTE could be described analytically and showed excellent accordance with numerical simulations. Even for tissues with T2 = 1 ms WE-UTE resulted in 79% of maximal signal yield of UTE without FatSat and was more efficient regarding signal yield if compared with UTE with FatSat. Using WE-UTE in-vivo tendons and ligaments could be well delineated with positive contrast to surrounding fat.


Conclusion
WE-UTE provides a quick method for visualizing short-T2 tissues with positive contrast. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24625" xmlns="http://purl.org/rss/1.0/"><title>Stages: Sub-Fourier dynamic shim updating using nonlinear magnetic field phase preparation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24625</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Stages: Sub-Fourier dynamic shim updating using nonlinear magnetic field phase preparation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Walter R. T. Witschey, Sebastian Littin, Chris A. Cocosco, Daniel Gallichan, Gerrit Schultz, Hans Weber, Anna Welz, Jürgen Hennig, Maxim Zaitsev</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T15:14:21.197512-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24625</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24625</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24625</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Heterogeneity of the static magnetic field in magnetic resonance imaging may cause image artifacts and degradation in image quality. The field heterogeneity can be reduced by dynamically adjusting shim fields or dynamic shim updating, in which magnetic field homogeneity is optimized for each tomographic slice to improve image quality. A limitation of this approach is that a new magnetic field can be applied only once for each slice, otherwise image quality would improve somewhere to its detriment elsewhere in the slice. The motivation of this work is to overcome this limitation and develop a technique using nonlinear magnetic fields to dynamically shim the static magnetic field within a single Fourier-encoded volume or slice, called sub-Fourier dynamic shim updating. However, the nonlinear magnetic fields are not used as shim fields; instead, they impart a strong spatial dependence to the acquired MR signal by nonlinear phase preparation, which may be exploited to locally improve magnetic field homogeneity during acquisition. A theoretical description of the method is detailed, simulations and a proof-of-principle experiment are performed using a magnet coil with a known field geometry. The method is shown to remove artifacts associated with magnetic field homogeneity in balanced steady-state free-precession pulse sequences. We anticipate that this method will be useful to improve the quality of magnetic resonance images by removing deleterious artifacts associated with a heterogeneous static magnetic field. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div>
]]></content:encoded><description>
Heterogeneity of the static magnetic field in magnetic resonance imaging may cause image artifacts and degradation in image quality. The field heterogeneity can be reduced by dynamically adjusting shim fields or dynamic shim updating, in which magnetic field homogeneity is optimized for each tomographic slice to improve image quality. A limitation of this approach is that a new magnetic field can be applied only once for each slice, otherwise image quality would improve somewhere to its detriment elsewhere in the slice. The motivation of this work is to overcome this limitation and develop a technique using nonlinear magnetic fields to dynamically shim the static magnetic field within a single Fourier-encoded volume or slice, called sub-Fourier dynamic shim updating. However, the nonlinear magnetic fields are not used as shim fields; instead, they impart a strong spatial dependence to the acquired MR signal by nonlinear phase preparation, which may be exploited to locally improve magnetic field homogeneity during acquisition. A theoretical description of the method is detailed, simulations and a proof-of-principle experiment are performed using a magnet coil with a known field geometry. The method is shown to remove artifacts associated with magnetic field homogeneity in balanced steady-state free-precession pulse sequences. We anticipate that this method will be useful to improve the quality of magnetic resonance images by removing deleterious artifacts associated with a heterogeneous static magnetic field. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24610" xmlns="http://purl.org/rss/1.0/"><title>Signal scaling improves the signal-to-noise ratio of measurements with segmented 2D-selective radiofrequency excitations</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24610</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Signal scaling improves the signal-to-noise ratio of measurements with segmented 2D-selective radiofrequency excitations</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jürgen Finsterbusch, Martin G. Busch, Peder E. Z. Larson</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T14:57:00.768843-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24610</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24610</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24610</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>Segmented 2D-selective radiofrequency excitations can be used to acquire irregularly shaped target regions, e.g., in single-voxel MR spectroscopy, without involving excessive radiofrequency pulse durations. However, segments covering only outer k-space regions nominally use reduced B1 amplitudes (i.e., smaller flip angles) and yield lower signal contributions, which decreases the efficiency of the measurement. The purpose of this study was to show that applying the full flip angle for all segments and scaling down the acquired signal appropriately (signal scaling) retains the desired signal amplitude but reduces the noise level accordingly and, thus, increases the signal-to-noise ratio.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>The principles and improvements of signal scaling were demonstrated with MR imaging and spectroscopy experiments at 3 T for a single-line segmentation of a blipped-planar trajectory.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>The observed signal-to-noise ration gain depended on the 2D-selective radiofrequency excitation's resolution, field-of-excitation, and its excitation profile and was between 40 and 500% for typical acquisition parameters.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>Signal scaling can further improve the performance of measurements with segmented 2D-selective radiofrequency excitations, e.g., for MR spectroscopy of anatomically defined voxels. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
Segmented 2D-selective radiofrequency excitations can be used to acquire irregularly shaped target regions, e.g., in single-voxel MR spectroscopy, without involving excessive radiofrequency pulse durations. However, segments covering only outer k-space regions nominally use reduced B1 amplitudes (i.e., smaller flip angles) and yield lower signal contributions, which decreases the efficiency of the measurement. The purpose of this study was to show that applying the full flip angle for all segments and scaling down the acquired signal appropriately (signal scaling) retains the desired signal amplitude but reduces the noise level accordingly and, thus, increases the signal-to-noise ratio.


Methods:
The principles and improvements of signal scaling were demonstrated with MR imaging and spectroscopy experiments at 3 T for a single-line segmentation of a blipped-planar trajectory.


Results:
The observed signal-to-noise ration gain depended on the 2D-selective radiofrequency excitation's resolution, field-of-excitation, and its excitation profile and was between 40 and 500% for typical acquisition parameters.


Conclusion:
Signal scaling can further improve the performance of measurements with segmented 2D-selective radiofrequency excitations, e.g., for MR spectroscopy of anatomically defined voxels. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24682" xmlns="http://purl.org/rss/1.0/"><title>Dynamic contrast-enhanced MRI in mice at high field: Estimation of the arterial input function can be achieved by phase imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24682</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Dynamic contrast-enhanced MRI in mice at high field: Estimation of the arterial input function can be achieved by phase imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A.-C. Fruytier, J. Magat, F. Colliez, B. Jordan, G. Cron, B. Gallez</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T12:20:26.450549-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24682</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24682</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24682</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24682-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Quantitative dynamic contrast-enhanced MRI requires an accurate arterial input function (AIF). At high field, increased susceptibility effects and decreased longitudinal relaxivity of contrast agents lead to predominant <em>T</em><sub>2</sub>* effects in blood vessels, producing a dip in signal during passage of the contrast agent bolus. This study determined phase-derived AIFs in mice at 11.7 T.</p></div></div>
<div class="section" id="mrm24682-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>AIFs were measured in aorta/vena cava for five FBV/N mice and in iliac arteries/veins for five NMRI mice with a fast low angle shot sequence, simultaneously with tumor imaging (temporal resolution: 1.19 s). Gadoterate was injected into the tail vein as a bolus (0.286 mmol Gd/kg). An in vitro study was also performed to calculate the relationship between ΔΦ and gadolinium concentration.</p></div></div>
<div class="section" id="mrm24682-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The phantom system confirmed the linear relationship between measured ΔΦ and gadolinium concentration. In vivo, a dip in arterial magnitude signal made it impossible to quantify the AIF. With phase imaging, a clear quantifiable bolus peak was obtained; peak measured concentration in plasma was 4.9 ± 0.9 mM for FBV/N mice and 8.0 ± 0.6 mM for NMRI mice, close to the expected concentration of 6.8 mM.</p></div></div>
<div class="section" id="mrm24682-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Phase imaging seems to be an appropriate means to measure the AIF of mice at high field. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Quantitative dynamic contrast-enhanced MRI requires an accurate arterial input function (AIF). At high field, increased susceptibility effects and decreased longitudinal relaxivity of contrast agents lead to predominant T2* effects in blood vessels, producing a dip in signal during passage of the contrast agent bolus. This study determined phase-derived AIFs in mice at 11.7 T.


Methods
AIFs were measured in aorta/vena cava for five FBV/N mice and in iliac arteries/veins for five NMRI mice with a fast low angle shot sequence, simultaneously with tumor imaging (temporal resolution: 1.19 s). Gadoterate was injected into the tail vein as a bolus (0.286 mmol Gd/kg). An in vitro study was also performed to calculate the relationship between ΔΦ and gadolinium concentration.


Results
The phantom system confirmed the linear relationship between measured ΔΦ and gadolinium concentration. In vivo, a dip in arterial magnitude signal made it impossible to quantify the AIF. With phase imaging, a clear quantifiable bolus peak was obtained; peak measured concentration in plasma was 4.9 ± 0.9 mM for FBV/N mice and 8.0 ± 0.6 mM for NMRI mice, close to the expected concentration of 6.8 mM.


Conclusion
Phase imaging seems to be an appropriate means to measure the AIF of mice at high field. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24676" xmlns="http://purl.org/rss/1.0/"><title>Orthogonalizing crusher and diffusion-encoding gradients to suppress undesired echo pathways in the twice-refocused spin echo diffusion sequence</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24676</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Orthogonalizing crusher and diffusion-encoding gradients to suppress undesired echo pathways in the twice-refocused spin echo diffusion sequence</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zoltán Nagy, David L. Thomas, Nikolaus Weiskopf</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T12:06:55.725029-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24676</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24676</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24676</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24676-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The twice-refocused spin echo sequence is widely used in diffusion imaging due to its excellent performance in reducing eddy currents. The three radio frequency pulses give rise to eight separate signal pathways. Because there is no general solution for the size and arrangement for crusher gradients, with constant size and orientation, that is effective for all arbitrary diffusion-sensitizing <em>b</em>-values and directions, this article introduces and validates a solution whereby the crusher and diffusion-encoding gradients are always kept orthogonal, thus ensuring their independence.</p></div></div>
<div class="section" id="mrm24676-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The cancellation of the crusher and diffusion gradients was demonstrated. Subsequently, crusher gradients were implemented in such a way that they were always orthogonal to the diffusion gradient. Phantom and in-vivo experiments were performed to ascertain that orthogonally implemented crusher gradients alleviate the problem without lowering image quality.</p></div></div>
<div class="section" id="mrm24676-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>In all experiments, when the crusher gradients' action was cancelled by the diffusion-encoding gradients artifactual signal modulation was observed. When orthogonal gradients were implemented the artifacts were eliminated without detrimental effects on image quality.</p></div></div>
<div class="section" id="mrm24676-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>Orthogonal crushers are easy to implement and can be used for any variant of diffusion imaging sequences (e.g., DTI, fiber diameter mapping) where the twice-refocused scheme is used. <b>Magn Reson Med, 2013.</b> © <b>2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
The twice-refocused spin echo sequence is widely used in diffusion imaging due to its excellent performance in reducing eddy currents. The three radio frequency pulses give rise to eight separate signal pathways. Because there is no general solution for the size and arrangement for crusher gradients, with constant size and orientation, that is effective for all arbitrary diffusion-sensitizing b-values and directions, this article introduces and validates a solution whereby the crusher and diffusion-encoding gradients are always kept orthogonal, thus ensuring their independence.


Methods
The cancellation of the crusher and diffusion gradients was demonstrated. Subsequently, crusher gradients were implemented in such a way that they were always orthogonal to the diffusion gradient. Phantom and in-vivo experiments were performed to ascertain that orthogonally implemented crusher gradients alleviate the problem without lowering image quality.


Results
In all experiments, when the crusher gradients' action was cancelled by the diffusion-encoding gradients artifactual signal modulation was observed. When orthogonal gradients were implemented the artifacts were eliminated without detrimental effects on image quality.


Conclusions
Orthogonal crushers are easy to implement and can be used for any variant of diffusion imaging sequences (e.g., DTI, fiber diameter mapping) where the twice-refocused scheme is used. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24683" xmlns="http://purl.org/rss/1.0/"><title>Accelerated isotropic sub-millimeter whole-heart coronary MRI: Compressed sensing versus parallel imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24683</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Accelerated isotropic sub-millimeter whole-heart coronary MRI: Compressed sensing versus parallel imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mehmet Akçakaya, Tamer A. Basha, Raymond H. Chan, Warren J. Manning, Reza Nezafat</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T12:02:02.380323-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24683</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24683</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24683</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24683-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To enable accelerated isotropic sub-millimeter whole-heart coronary MRI within a 6-min acquisition and to compare this with a current state-of-the-art accelerated imaging technique at acceleration rates beyond what is used clinically.</p></div></div>
<div class="section" id="mrm24683-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Coronary MRI still faces major challenges, including lengthy acquisition time, low signal-to-noise-ratio (SNR), and suboptimal spatial resolution. Higher spatial resolution in the sub-millimeter range is desirable, but this results in increased acquisition time and lower SNR, hindering its clinical implementation. In this study, we sought to use an advanced <em>B</em><sub>1</sub>-weighted compressed sensing technique for highly accelerated sub-millimeter whole-heart coronary MRI, and to compare the results to parallel imaging, the current-state-of-the-art, where both techniques were used at acceleration rates beyond what is used clinically. Two whole-heart coronary MRI datasets were acquired in seven healthy adult subjects (30.3 ± 12.1 years; 3 men), using prospective 6-fold acceleration, with random undersampling for the proposed compressed sensing technique and with uniform undersampling for sensitivity encoding reconstruction. Reconstructed images were qualitatively compared in terms of image scores and perceived SNR on a four-point scale (1 = poor, 4 = excellent) by an experienced blinded reader.</p></div></div>
<div class="section" id="mrm24683-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The proposed technique resulted in images with clear visualization of all coronary branches. Overall image quality and perceived SNR of the compressed sensing images were significantly higher than those of parallel imaging (<em>P</em> = 0.03 for both), which suffered from noise amplification artifacts due to the reduced SNR.</p></div></div>
<div class="section" id="mrm24683-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The proposed compressed sensing-based reconstruction and acquisition technique for sub-millimeter whole-heart coronary MRI provides 6-fold acceleration, where it outperforms parallel imaging with uniform undersampling. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
To enable accelerated isotropic sub-millimeter whole-heart coronary MRI within a 6-min acquisition and to compare this with a current state-of-the-art accelerated imaging technique at acceleration rates beyond what is used clinically.


Methods
Coronary MRI still faces major challenges, including lengthy acquisition time, low signal-to-noise-ratio (SNR), and suboptimal spatial resolution. Higher spatial resolution in the sub-millimeter range is desirable, but this results in increased acquisition time and lower SNR, hindering its clinical implementation. In this study, we sought to use an advanced B1-weighted compressed sensing technique for highly accelerated sub-millimeter whole-heart coronary MRI, and to compare the results to parallel imaging, the current-state-of-the-art, where both techniques were used at acceleration rates beyond what is used clinically. Two whole-heart coronary MRI datasets were acquired in seven healthy adult subjects (30.3 ± 12.1 years; 3 men), using prospective 6-fold acceleration, with random undersampling for the proposed compressed sensing technique and with uniform undersampling for sensitivity encoding reconstruction. Reconstructed images were qualitatively compared in terms of image scores and perceived SNR on a four-point scale (1 = poor, 4 = excellent) by an experienced blinded reader.


Results
The proposed technique resulted in images with clear visualization of all coronary branches. Overall image quality and perceived SNR of the compressed sensing images were significantly higher than those of parallel imaging (P = 0.03 for both), which suffered from noise amplification artifacts due to the reduced SNR.


Conclusion
The proposed compressed sensing-based reconstruction and acquisition technique for sub-millimeter whole-heart coronary MRI provides 6-fold acceleration, where it outperforms parallel imaging with uniform undersampling. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24689" xmlns="http://purl.org/rss/1.0/"><title>Time-resolved noncontrast enhanced 4-D dynamic magnetic resonance angiography using multibolus TrueFISP-based spin tagging with alternating radiofrequency (TrueSTAR)</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24689</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Time-resolved noncontrast enhanced 4-D dynamic magnetic resonance angiography using multibolus TrueFISP-based spin tagging with alternating radiofrequency (TrueSTAR)</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lirong Yan, Noriko Salamon, Danny J. J. Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T12:01:59.177895-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24689</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24689</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24689</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24689-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The goal of this study was to introduce a new noncontrast enhanced 4D dynamic MR angiography (dMRA) technique termed multibolus TrueFISP-based spin tagging with alternating radiofrequency (TrueSTAR).</p></div></div>
<div class="section" id="mrm24689-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Multibolus TrueFISP-based spin tagging with alternating radiofrequency was developed by taking advantage of the phenomenon that the steady-state signal of TrueFISP is minimally disturbed by periodically inserted magnetization preparations (e.g., spin tagging) that are sandwiched by two <em>α</em>/2 RF pulses. Both theoretical analysis and experimental studies were carried out to optimize the proposed method which was compared with both pulsed and pseudo-continuous arterial spin labeling-based dMRA in healthy volunteers. Optimized multibolus dMRA was also applied in a patient with arteriovenous malformation to demonstrate its potential clinical utility.</p></div></div>
<div class="section" id="mrm24689-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Multibolus dMRA offered a prolonged tagging bolus compared to the standard single-bolus dMRA, and allowed improved visualization of the draining veins in the arteriovenous malformation patient. Compared to pseudo-continuous arterial spin labeling-based dMRA, multibolus dMRA provided visualization of the full passage of the labeled blood with the flexibility for both static and dynamic magnetic resonance angiography.</p></div></div>
<div class="section" id="mrm24689-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>By combining the benefits of pulsed and pseudo-continuous arterial spin labeling-based dMRA, multibolus TrueFISP-based spin tagging with alternating radiofrequency can prolong and enhance the tagging bolus without sacrificing imaging speed or temporal resolution. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The goal of this study was to introduce a new noncontrast enhanced 4D dynamic MR angiography (dMRA) technique termed multibolus TrueFISP-based spin tagging with alternating radiofrequency (TrueSTAR).


Methods
Multibolus TrueFISP-based spin tagging with alternating radiofrequency was developed by taking advantage of the phenomenon that the steady-state signal of TrueFISP is minimally disturbed by periodically inserted magnetization preparations (e.g., spin tagging) that are sandwiched by two α/2 RF pulses. Both theoretical analysis and experimental studies were carried out to optimize the proposed method which was compared with both pulsed and pseudo-continuous arterial spin labeling-based dMRA in healthy volunteers. Optimized multibolus dMRA was also applied in a patient with arteriovenous malformation to demonstrate its potential clinical utility.


Results
Multibolus dMRA offered a prolonged tagging bolus compared to the standard single-bolus dMRA, and allowed improved visualization of the draining veins in the arteriovenous malformation patient. Compared to pseudo-continuous arterial spin labeling-based dMRA, multibolus dMRA provided visualization of the full passage of the labeled blood with the flexibility for both static and dynamic magnetic resonance angiography.


Conclusion
By combining the benefits of pulsed and pseudo-continuous arterial spin labeling-based dMRA, multibolus TrueFISP-based spin tagging with alternating radiofrequency can prolong and enhance the tagging bolus without sacrificing imaging speed or temporal resolution. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24688" xmlns="http://purl.org/rss/1.0/"><title>3D myocardial T1 mapping at 3T using variable flip angle method: Pilot study</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24688</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">3D myocardial T1 mapping at 3T using variable flip angle method: Pilot study</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hélène Clique, Hai-Ling Margaret Cheng, Pierre-Yves Marie, Jacques Felblinger, Marine Beaumont</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T12:01:41.567322-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24688</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24688</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24688</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24688-sec-0015" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Myocardial <em>T</em><sub>1</sub> mapping is an emerging technique that could improve cardiovascular magnetic resonance diagnostic accuracy. In this study, a variable flip angle approach with B<sub>1</sub> correction is proposed at 3T on the myocardium, employing standard 3D spoiled fast gradient echo and echo planar imaging sequences.</p></div></div>
<div class="section" id="mrm24688-sec-0016" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The method was tested on phantoms to determine the set of standard 3D spoiled fast gradient echo angles adapted to myocardial <em>T</em><sub>1</sub> measurements and was compared to the inversion-recovery spin-echo reference <em>T</em><sub>1</sub> method. Seven volunteers underwent magnetic imaging resonance to acquire myocardial <em>T</em><sub>1</sub> maps and <em>T</em><sub>1</sub> values of the human heart.</p></div></div>
<div class="section" id="mrm24688-sec-0017" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>This original method demonstrated good reproducibility in phantoms and a significant correlation between variable flip angle <em>T</em><sub>1</sub> values and reference inversion-recovery spin-echo <em>T</em><sub>1</sub> values. It yielded myocardial <em>T</em><sub>1</sub> values consistent with expected <em>T</em><sub>1</sub> and an increasing homogenization of myocardial segments owing to <em>B</em><sub>1</sub> correction. The mean myocardial <em>T</em><sub>1</sub> value was 1341 ± 42 ms.</p></div></div>
<div class="section" id="mrm24688-sec-0014" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Myocardial 3D <em>T</em><sub>1</sub> mapping using the variable flip angle approach can potentially be useful for evaluating fibrosis on the entire myocardium using a standard clinical sequence. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Myocardial T1 mapping is an emerging technique that could improve cardiovascular magnetic resonance diagnostic accuracy. In this study, a variable flip angle approach with B1 correction is proposed at 3T on the myocardium, employing standard 3D spoiled fast gradient echo and echo planar imaging sequences.


Methods
The method was tested on phantoms to determine the set of standard 3D spoiled fast gradient echo angles adapted to myocardial T1 measurements and was compared to the inversion-recovery spin-echo reference T1 method. Seven volunteers underwent magnetic imaging resonance to acquire myocardial T1 maps and T1 values of the human heart.


Results
This original method demonstrated good reproducibility in phantoms and a significant correlation between variable flip angle T1 values and reference inversion-recovery spin-echo T1 values. It yielded myocardial T1 values consistent with expected T1 and an increasing homogenization of myocardial segments owing to B1 correction. The mean myocardial T1 value was 1341 ± 42 ms.


Conclusion
Myocardial 3D T1 mapping using the variable flip angle approach can potentially be useful for evaluating fibrosis on the entire myocardium using a standard clinical sequence. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24644" xmlns="http://purl.org/rss/1.0/"><title>Analysis of image heterogeneity using 2D Minkowski functionals detects tumor responses to treatment</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24644</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Analysis of image heterogeneity using 2D Minkowski functionals detects tumor responses to treatment</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Timothy J. Larkin, Holly C. Canuto, Mikko I. Kettunen, Thomas C. Booth, De-En Hu, Anant S. Krishnan, Sarah E. Bohndiek, André A. Neves, Charles McLachlan, Michael P. Hobson, Kevin M. Brindle</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T12:01:36.322195-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24644</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24644</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24644</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24644-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The acquisition of ever increasing volumes of high resolution magnetic resonance imaging (MRI) data has created an urgent need to develop automated and objective image analysis algorithms that can assist in determining tumor margins, diagnosing tumor stage, and detecting treatment response.</p></div></div>
<div class="section" id="mrm24644-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>We have shown previously that Minkowski functionals, which are precise morphological and structural descriptors of image heterogeneity, can be used to enhance the detection, in <em>T</em><sub>1</sub>-weighted images, of a targeted Gd<sup>3+</sup>-chelate-based contrast agent for detecting tumor cell death. We have used Minkowski functionals here to characterize heterogeneity in <em>T</em><sub>2</sub>-weighted images acquired before and after drug treatment, and obtained without contrast agent administration.</p></div></div>
<div class="section" id="mrm24644-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>We show that Minkowski functionals can be used to characterize the changes in image heterogeneity that accompany treatment of tumors with a vascular disrupting agent, combretastatin A4-phosphate, and with a cytotoxic drug, etoposide.</p></div></div>
<div class="section" id="mrm24644-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>Parameterizing changes in the heterogeneity of <em>T</em><sub>2</sub>-weighted images can be used to detect early responses of tumors to drug treatment, even when there is no change in tumor size. The approach provides a quantitative and therefore objective assessment of treatment response that could be used with other types of MR image and also with other imaging modalities.</p></div></div>
]]></content:encoded><description>

Purpose
The acquisition of ever increasing volumes of high resolution magnetic resonance imaging (MRI) data has created an urgent need to develop automated and objective image analysis algorithms that can assist in determining tumor margins, diagnosing tumor stage, and detecting treatment response.


Methods
We have shown previously that Minkowski functionals, which are precise morphological and structural descriptors of image heterogeneity, can be used to enhance the detection, in T1-weighted images, of a targeted Gd3+-chelate-based contrast agent for detecting tumor cell death. We have used Minkowski functionals here to characterize heterogeneity in T2-weighted images acquired before and after drug treatment, and obtained without contrast agent administration.


Results
We show that Minkowski functionals can be used to characterize the changes in image heterogeneity that accompany treatment of tumors with a vascular disrupting agent, combretastatin A4-phosphate, and with a cytotoxic drug, etoposide.


Conclusions
Parameterizing changes in the heterogeneity of T2-weighted images can be used to detect early responses of tumors to drug treatment, even when there is no change in tumor size. The approach provides a quantitative and therefore objective assessment of treatment response that could be used with other types of MR image and also with other imaging modalities.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24686" xmlns="http://purl.org/rss/1.0/"><title>Application of direct virtual coil to dynamic contrast-enhanced MRI and MR angiography with data-driven parallel imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24686</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Application of direct virtual coil to dynamic contrast-enhanced MRI and MR angiography with data-driven parallel imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kang Wang, Philip J. Beatty, Scott K. Nagle, Scott B. Reeder, James H. Holmes, Mahdi S. Rahimi, Laura C. Bell, Frank R. Korosec, Jean H. Brittain</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T12:01:02.882483-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24686</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24686</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24686</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24686-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To demonstrate the feasibility of direct virtual coil (DVC) in the setting of 4D dynamic imaging used in multiple clinical applications.</p></div></div>
<div class="section" id="mrm24686-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>Three dynamic imaging applications were chosen: pulmonary perfusion, liver perfusion, and peripheral MR angiography (MRA), with 18, 11, and 10 subjects, respectively. After view-sharing, the k-space data were reconstructed twice: once with channel-by-channel (CBC) followed by sum-of-squares coil combination and once with DVC. Images reconstructed using CBC and DVC were compared and scored based on overall image quality by two experienced radiologists using a five-point scale.</p></div></div>
<div class="section" id="mrm24686-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The CBC and DVC showed similar image quality in image domain. Time course measurements also showed good agreement in the temporal domain. CBC and DVC images were scored as equivalent for all pulmonary perfusion cases, all liver perfusion cases, and four of the 10 peripheral MRA cases. For the remaining six peripheral MRA cases, DVC were scored as slightly better (not clinically significant) than the CBC images by Radiologist A and as equivalent by Radiologist B.</p></div></div>
<div class="section" id="mrm24686-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>For dynamic contrast-enhanced MR applications, it is clinically feasible to reduce image reconstruction time while maintaining image quality and time course measurement using the DVC technique.<b> Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc</b>.</p></div></div>
]]></content:encoded><description>

Purpose
To demonstrate the feasibility of direct virtual coil (DVC) in the setting of 4D dynamic imaging used in multiple clinical applications.


Theory and Methods
Three dynamic imaging applications were chosen: pulmonary perfusion, liver perfusion, and peripheral MR angiography (MRA), with 18, 11, and 10 subjects, respectively. After view-sharing, the k-space data were reconstructed twice: once with channel-by-channel (CBC) followed by sum-of-squares coil combination and once with DVC. Images reconstructed using CBC and DVC were compared and scored based on overall image quality by two experienced radiologists using a five-point scale.


Results
The CBC and DVC showed similar image quality in image domain. Time course measurements also showed good agreement in the temporal domain. CBC and DVC images were scored as equivalent for all pulmonary perfusion cases, all liver perfusion cases, and four of the 10 peripheral MRA cases. For the remaining six peripheral MRA cases, DVC were scored as slightly better (not clinically significant) than the CBC images by Radiologist A and as equivalent by Radiologist B.


Conclusion
For dynamic contrast-enhanced MR applications, it is clinically feasible to reduce image reconstruction time while maintaining image quality and time course measurement using the DVC technique. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24677" xmlns="http://purl.org/rss/1.0/"><title>Analysis and correction of biases in cross-relaxation MRI due to biexponential longitudinal relaxation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24677</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Analysis and correction of biases in cross-relaxation MRI due to biexponential longitudinal relaxation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Pouria Mossahebi, Vasily L. Yarnykh, Alexey Samsonov</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T12:00:02.12618-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24677</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24677</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24677</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24677-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Cross-relaxation imaging (CRI) is a family of quantitative magnetization transfer techniques that utilize images obtained with off-resonance saturation and longitudinal relaxation rate (<em>R</em><sub>1</sub>) maps reconstructed by the variable flip angle (VFA) method. It was demonstrated recently that a significant bias in an apparent VFA <em>R</em><sub>1</sub> estimation occurs in macromolecule-rich tissues due to magnetization transfer-induced biexponential behavior of longitudinal relaxation of water protons. The purpose of this article is to characterize theoretically and experimentally the resulting bias in the CRI maps and propose methods to correct it.</p></div></div>
<div class="section" id="mrm24677-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory</h4><div class="para"><p>The modified CRI algorithm is proposed, which corrects for such biases and yields accurate parametric bound pool fraction <em>f</em>, cross-relaxation rate <em>k</em>, and <em>R</em><sub>1</sub> maps. Additionally, an analytical correction procedure is introduced to recalculate previously obtained parameter values.</p></div></div>
<div class="section" id="mrm24677-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The systematic errors due to unaccounted biexponential relaxation can be characterized as an overestimation of <em>R</em><sub>1</sub>, <em>f</em>, and <em>k</em>, with a relative bias comparable with the magnitude of <em>f</em>. The phantom and human in vivo experiments demonstrate that both proposed modified CRI and analytical correction approaches significantly improve the accuracy of the CRI method.</p></div></div>
<div class="section" id="mrm24677-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The accuracy of the CRI method can be considerably improved by taking into account the contribution of magnetization transfer-induced biexponential longitudinal relaxation into variable flip angle <em>R</em><sub>1</sub> measurements. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Cross-relaxation imaging (CRI) is a family of quantitative magnetization transfer techniques that utilize images obtained with off-resonance saturation and longitudinal relaxation rate (R1) maps reconstructed by the variable flip angle (VFA) method. It was demonstrated recently that a significant bias in an apparent VFA R1 estimation occurs in macromolecule-rich tissues due to magnetization transfer-induced biexponential behavior of longitudinal relaxation of water protons. The purpose of this article is to characterize theoretically and experimentally the resulting bias in the CRI maps and propose methods to correct it.


Theory
The modified CRI algorithm is proposed, which corrects for such biases and yields accurate parametric bound pool fraction f, cross-relaxation rate k, and R1 maps. Additionally, an analytical correction procedure is introduced to recalculate previously obtained parameter values.


Results
The systematic errors due to unaccounted biexponential relaxation can be characterized as an overestimation of R1, f, and k, with a relative bias comparable with the magnitude of f. The phantom and human in vivo experiments demonstrate that both proposed modified CRI and analytical correction approaches significantly improve the accuracy of the CRI method.


Conclusion
The accuracy of the CRI method can be considerably improved by taking into account the contribution of magnetization transfer-induced biexponential longitudinal relaxation into variable flip angle R1 measurements. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24679" xmlns="http://purl.org/rss/1.0/"><title>Knee cartilage MRI with in situ mechanical loading using prospective motion correction</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24679</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Knee cartilage MRI with in situ mechanical loading using prospective motion correction</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Thomas Lange, Julian Maclaren, Michael Herbst, Cris Lovell-Smith, Kaywan Izadpanah, Maxim Zaitsev</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T11:59:12.588873-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24679</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24679</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24679</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24679-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To assess the feasibility of high resolution knee cartilage MRI with in situ mechanical loading using optical tracking to compensate for motion.</p></div></div>
<div class="section" id="mrm24679-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>In vivo cartilage MRI with in situ mechanical loading is demonstrated on a clinical 3T system for the patellofemoral as well as for the tibiofemoral knee joint using a <em>T</em><sub>1</sub>-weighted spoiled three-dimensional gradient-echo sequence. Prospective motion correction is performed with a moiré phase tracking system consisting of an in-bore camera and a single tracking marker attached to the skin.</p></div></div>
<div class="section" id="mrm24679-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Rigid-body approximation required for prospective correction with optical motion tracking is fulfilled well enough for the patellofemoral as well as for the tibiofemoral joint when the tracking marker is attached to the knee cap and the shin, respectively. Presaturation proves to be efficient in suppressing pulsation artifacts from the popliteal artery and residual motion artifacts primarily arising from nonrigid motion of the posterior knee compartment.</p></div></div>
<div class="section" id="mrm24679-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The proposed technique enables knee cartilage imaging under in situ mechanical loading with submillimeter spatial resolution devoid of significant motion artifacts and thus appropriate for cartilage volumetry. It has the potential to provide new insight into the biomechanics of the knee and might complement the panoply of diagnostic MR methods for osteoarthritis. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To assess the feasibility of high resolution knee cartilage MRI with in situ mechanical loading using optical tracking to compensate for motion.


Methods
In vivo cartilage MRI with in situ mechanical loading is demonstrated on a clinical 3T system for the patellofemoral as well as for the tibiofemoral knee joint using a T1-weighted spoiled three-dimensional gradient-echo sequence. Prospective motion correction is performed with a moiré phase tracking system consisting of an in-bore camera and a single tracking marker attached to the skin.


Results
Rigid-body approximation required for prospective correction with optical motion tracking is fulfilled well enough for the patellofemoral as well as for the tibiofemoral joint when the tracking marker is attached to the knee cap and the shin, respectively. Presaturation proves to be efficient in suppressing pulsation artifacts from the popliteal artery and residual motion artifacts primarily arising from nonrigid motion of the posterior knee compartment.


Conclusion
The proposed technique enables knee cartilage imaging under in situ mechanical loading with submillimeter spatial resolution devoid of significant motion artifacts and thus appropriate for cartilage volumetry. It has the potential to provide new insight into the biomechanics of the knee and might complement the panoply of diagnostic MR methods for osteoarthritis. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24638" xmlns="http://purl.org/rss/1.0/"><title>Steady-state first-pass perfusion (SSFPP): A new approach to 3D first-pass myocardial perfusion imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24638</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Steady-state first-pass perfusion (SSFPP): A new approach to 3D first-pass myocardial perfusion imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Shivraman Giri, Hui Xue, Andrei Maiseyeu, Randall Kroeker, Sanjay Rajagopalan, Richard D. White, Sven Zuehlsdorff, Subha V. Raman, Orlando P. Simonetti</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T11:57:14.772588-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24638</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24638</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24638</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24638-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To describe and characterize a new approach to first-pass myocardial perfusion utilizing balanced steady-state free precession acquisition without the use of saturation recovery or other magnetization preparation.</p></div></div>
<div class="section" id="mrm24638-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory</h4><div class="para"><p>The balanced steady-state free precession sequence is inherently sensitive to contrast agent enhancement of the myocardium. This sensitivity can be used to advantage in first-pass myocardial perfusion imaging by eliminating the need for magnetization preparation.</p></div></div>
<div class="section" id="mrm24638-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Bloch equation simulations, phantom experiments, and in vivo 2D imaging studies were run comparing the proposed technique with three other methods: saturation recovery spoiled gradient echo, saturation recovery steady-state free precession, and steady-state spoiled gradient echo without magnetization preparation. Additionally, an acquisition-reconstruction strategy for 3D perfusion imaging is proposed and initial experience with this approach is demonstrated in healthy subjects and one patient.</p></div></div>
<div class="section" id="mrm24638-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Phantom experiments verified simulation results showing the sensitivity of the balanced steady-state free precession sequence to contrast agent enhancement in solid tissue is similar to that of magnetization-prepared acquisitions. Images acquired in normal volunteers showed the proposed technique provided superior signal and signal-to-noise ratio compared with all other sequences at baseline as well as postcontrast.</p></div></div>
<div class="section" id="mrm24638-sec-0005" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>A new approach to first-pass myocardial perfusion is presented that obviates the need for magnetization preparation and provides high signal-to-noise ratio. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To describe and characterize a new approach to first-pass myocardial perfusion utilizing balanced steady-state free precession acquisition without the use of saturation recovery or other magnetization preparation.


Theory
The balanced steady-state free precession sequence is inherently sensitive to contrast agent enhancement of the myocardium. This sensitivity can be used to advantage in first-pass myocardial perfusion imaging by eliminating the need for magnetization preparation.


Methods
Bloch equation simulations, phantom experiments, and in vivo 2D imaging studies were run comparing the proposed technique with three other methods: saturation recovery spoiled gradient echo, saturation recovery steady-state free precession, and steady-state spoiled gradient echo without magnetization preparation. Additionally, an acquisition-reconstruction strategy for 3D perfusion imaging is proposed and initial experience with this approach is demonstrated in healthy subjects and one patient.


Results
Phantom experiments verified simulation results showing the sensitivity of the balanced steady-state free precession sequence to contrast agent enhancement in solid tissue is similar to that of magnetization-prepared acquisitions. Images acquired in normal volunteers showed the proposed technique provided superior signal and signal-to-noise ratio compared with all other sequences at baseline as well as postcontrast.


Conclusions
A new approach to first-pass myocardial perfusion is presented that obviates the need for magnetization preparation and provides high signal-to-noise ratio. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24661" xmlns="http://purl.org/rss/1.0/"><title>Ex vivo MR volumetry of human brain hemispheres</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24661</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Ex vivo MR volumetry of human brain hemispheres</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Aikaterini Kotrotsou, David A. Bennett, Julie A. Schneider, Robert J. Dawe, Tom Golak, Sue E. Leurgans, Lei Yu, Konstantinos Arfanakis</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T11:52:19.790508-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24661</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24661</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24661</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24661-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The aims of this work were to (a) develop an approach for ex vivo MR volumetry of human brain hemispheres that does not contaminate the results of histopathological examination, (b) longitudinally assess regional brain volumes postmortem, and (c) investigate the relationship between MR volumetric measurements performed in vivo and ex vivo.</p></div></div>
<div class="section" id="mrm24661-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>An approach for ex vivo MR volumetry of human brain hemispheres was developed. Five hemispheres from elderly subjects were imaged ex vivo longitudinally. All datasets were segmented. The longitudinal behavior of volumes measured ex vivo was assessed. The relationship between in vivo and ex vivo volumetric measurements was investigated in seven elderly subjects imaged both antemortem and postmortem.</p></div></div>
<div class="section" id="mrm24661-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>This approach for ex vivo MR volumetry did not contaminate the results of histopathological examination. For a period of 6 months postmortem, within-subject volume variation across time points was substantially smaller than intersubject volume variation. A close linear correspondence was detected between in vivo and ex vivo volumetric measurements.</p></div></div>
<div class="section" id="mrm24661-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Regional brain volumes measured with this approach for ex vivo MR volumetry remain relatively unchanged for a period of 6 months postmortem. Furthermore, the linear relationship between in vivo and ex vivo MR volumetric measurements suggests that this approach captures information linked to antemortem macrostructural brain characteristics. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The aims of this work were to (a) develop an approach for ex vivo MR volumetry of human brain hemispheres that does not contaminate the results of histopathological examination, (b) longitudinally assess regional brain volumes postmortem, and (c) investigate the relationship between MR volumetric measurements performed in vivo and ex vivo.


Methods
An approach for ex vivo MR volumetry of human brain hemispheres was developed. Five hemispheres from elderly subjects were imaged ex vivo longitudinally. All datasets were segmented. The longitudinal behavior of volumes measured ex vivo was assessed. The relationship between in vivo and ex vivo volumetric measurements was investigated in seven elderly subjects imaged both antemortem and postmortem.


Results
This approach for ex vivo MR volumetry did not contaminate the results of histopathological examination. For a period of 6 months postmortem, within-subject volume variation across time points was substantially smaller than intersubject volume variation. A close linear correspondence was detected between in vivo and ex vivo volumetric measurements.


Conclusion
Regional brain volumes measured with this approach for ex vivo MR volumetry remain relatively unchanged for a period of 6 months postmortem. Furthermore, the linear relationship between in vivo and ex vivo MR volumetric measurements suggests that this approach captures information linked to antemortem macrostructural brain characteristics. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24626" xmlns="http://purl.org/rss/1.0/"><title>Initial clinical evaluation of a non-contrast-enhanced MR angiography method in the distal lower extremities</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24626</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Initial clinical evaluation of a non-contrast-enhanced MR angiography method in the distal lower extremities</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Andrew Nicholas Priest, Ilse Joubert, Andrew Philip Winterbottom, Teik Choon See, Martin John Graves, David John Lomas</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-25T09:39:14.903767-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24626</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24626</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24626</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24626-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To report the initial experience and diagnostic performance applying a novel flow-dependent non-contrast-enhanced MR angiography (NCE-MRA) method, in patients with suspected peripheral vascular disease, in comparison with established contrast-enhanced MRA (CE-MRA).</p></div></div>
<div class="section" id="mrm24626-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The lower legs of 34 patients were imaged at 1.5 T with both NCE-MRA and CE-MRA. The NCE-MRA method consisted of a cardiac-gated balanced-SSFP sequence with controllable flow-suppression preparation. Flow-suppressed and unsuppressed datasets were subtracted to obtain angiograms. Two experienced radiologists assessed both NCE-MRA and CE-MRA images, first independently and then in consensus to resolve significant disagreements. Signal loss, vessel conspicuity, vascular disease, venous contamination, artifacts, and diagnostic confidence were assessed.</p></div></div>
<div class="section" id="mrm24626-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Using the CE-MRA as the “gold standard,” the per-segment sensitivity and specificity for detection of significant disease were 81.7% and 90.9%, respectively. Mean diagnostic confidence (scale 0–4) was 3.4 for NCE-MRA and 3.9 for CE-MRA. Most vessel segments were well visualized but the popliteal arteries often suffered some technique-related signal loss.</p></div></div>
<div class="section" id="mrm24626-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>The NCE-MRA method was able to visualize most vessel segments with good or excellent confidence, few artifacts, and excellent background suppression, giving moderate agreement with CE-MRA. However, some segments were poorly visualized, probably due to flow profile distortion in these patients. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
To report the initial experience and diagnostic performance applying a novel flow-dependent non-contrast-enhanced MR angiography (NCE-MRA) method, in patients with suspected peripheral vascular disease, in comparison with established contrast-enhanced MRA (CE-MRA).


Methods
The lower legs of 34 patients were imaged at 1.5 T with both NCE-MRA and CE-MRA. The NCE-MRA method consisted of a cardiac-gated balanced-SSFP sequence with controllable flow-suppression preparation. Flow-suppressed and unsuppressed datasets were subtracted to obtain angiograms. Two experienced radiologists assessed both NCE-MRA and CE-MRA images, first independently and then in consensus to resolve significant disagreements. Signal loss, vessel conspicuity, vascular disease, venous contamination, artifacts, and diagnostic confidence were assessed.


Results
Using the CE-MRA as the “gold standard,” the per-segment sensitivity and specificity for detection of significant disease were 81.7% and 90.9%, respectively. Mean diagnostic confidence (scale 0–4) was 3.4 for NCE-MRA and 3.9 for CE-MRA. Most vessel segments were well visualized but the popliteal arteries often suffered some technique-related signal loss.


Conclusions
The NCE-MRA method was able to visualize most vessel segments with good or excellent confidence, few artifacts, and excellent background suppression, giving moderate agreement with CE-MRA. However, some segments were poorly visualized, probably due to flow profile distortion in these patients. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24669" xmlns="http://purl.org/rss/1.0/"><title>Noncontrast skeletal muscle oximetry</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24669</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Noncontrast skeletal muscle oximetry</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jie Zheng, Hongyu An, Andrew R. Coggan, Xiaodong Zhang, Adil Bashir, David Muccigrosso, Linda R. Peterson, Robert J. Gropler</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-19T13:11:37.01224-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24669</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24669</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24669</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24669-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The objective of this study was to develop a new noncontrast method to directly quantify regional skeletal muscle oxygenation.</p></div></div>
<div class="section" id="mrm24669-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The feasibility of the method was examined in five healthy volunteers using a 3 T clinical MRI scanner, at rest and during a sustained isometric contraction. The perfusion of skeletal muscle of the calf was measured using an arterial spin labeling method, whereas the oxygen extraction fraction of the muscle was measured using a susceptibility-based MRI technique.</p></div></div>
<div class="section" id="mrm24669-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>In all volunteers, the perfusion in soleus muscle increased significantly from 6.5 ± 2.0 mL (100 g min)<sup>−1</sup> at rest to 47.9 ± 7.7 mL (100 g min)<sup>−1</sup> during exercise (<em>P</em> &lt; 0.05). Although the corresponding oxygen extraction fraction did not change significantly, the rate of oxygen consumption increased from 0.43 ± 0.13 to 4.2 ± 1.5 mL (100 g min)<sup>−1</sup> (<em>P</em> &lt; 0.05). Similar results were observed in gastrocnemius muscle but with greater oxygen extraction fraction increase than the soleus muscle.</p></div></div>
<div class="section" id="mrm24669-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>This is the first MR oximetry developed for quantification of regional skeletal muscle oxygenation. A broad range of medical conditions could benefit from these techniques, including cardiology, gerontology, kinesiology, and physical therapy. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
The objective of this study was to develop a new noncontrast method to directly quantify regional skeletal muscle oxygenation.


Methods
The feasibility of the method was examined in five healthy volunteers using a 3 T clinical MRI scanner, at rest and during a sustained isometric contraction. The perfusion of skeletal muscle of the calf was measured using an arterial spin labeling method, whereas the oxygen extraction fraction of the muscle was measured using a susceptibility-based MRI technique.


Results
In all volunteers, the perfusion in soleus muscle increased significantly from 6.5 ± 2.0 mL (100 g min)−1 at rest to 47.9 ± 7.7 mL (100 g min)−1 during exercise (P &lt; 0.05). Although the corresponding oxygen extraction fraction did not change significantly, the rate of oxygen consumption increased from 0.43 ± 0.13 to 4.2 ± 1.5 mL (100 g min)−1 (P &lt; 0.05). Similar results were observed in gastrocnemius muscle but with greater oxygen extraction fraction increase than the soleus muscle.


Conclusion
This is the first MR oximetry developed for quantification of regional skeletal muscle oxygenation. A broad range of medical conditions could benefit from these techniques, including cardiology, gerontology, kinesiology, and physical therapy. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24666" xmlns="http://purl.org/rss/1.0/"><title>Early postsurgical visualization of composite mesh used in ventral hernia repair by amide proton transfer MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24666</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Early postsurgical visualization of composite mesh used in ventral hernia repair by amide proton transfer MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Florence Franconi, Jérome Roux, Xavier Garric, Laurent Lemaire</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-19T13:10:59.433259-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24666</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24666</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24666</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24666-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The feasibility of noninvasive visualization of composite meshes used in ventral hernia repair by amide-proton transfer magnetic resonance imaging (APT-MRI) was explored.</p></div></div>
<div class="section" id="mrm24666-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Magnetization transfer asymmetry ratio images of composite meshes were obtained in vitro and in vivo from fast-spin echo acquisitions with frequency saturation offsets of ±3.5 ppm with respect to water frequency and no saturation. Three rats were assessed with APT-MRI each week for 1 month after the intraperitoneal implantation of two meshes, one on each side of the incision. One mesh was coated with collagen and the other was not.</p></div></div>
<div class="section" id="mrm24666-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>In vitro, meshes were delineated with APT-MRI as a thin continuous linear hypersignal located on one side of the mesh. Unlike collagen-free meshes, collagen-coated meshes were easily identified in vivo with APT-MRI during the first 3 weeks postimplantation. The composite meshes magnetization transfer asymmetry ratio (8.7 ± 2.8%) were significantly different from the muscle magnetization transfer asymmetry ratio value (−0.9 ± 1.6%). After a month, the mesh value dropped down to 1.1 ± 3.9%. Muscle and mesh magnetization transfer asymmetry ratio values were not significantly different and mesh conspicuity was no longer possible.</p></div></div>
<div class="section" id="mrm24666-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The results suggest that APT-MRI is a promising technique for noninvasive, early postsurgical visualization of composite meshes used in ventral hernia repair. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
The feasibility of noninvasive visualization of composite meshes used in ventral hernia repair by amide-proton transfer magnetic resonance imaging (APT-MRI) was explored.


Methods
Magnetization transfer asymmetry ratio images of composite meshes were obtained in vitro and in vivo from fast-spin echo acquisitions with frequency saturation offsets of ±3.5 ppm with respect to water frequency and no saturation. Three rats were assessed with APT-MRI each week for 1 month after the intraperitoneal implantation of two meshes, one on each side of the incision. One mesh was coated with collagen and the other was not.


Results
In vitro, meshes were delineated with APT-MRI as a thin continuous linear hypersignal located on one side of the mesh. Unlike collagen-free meshes, collagen-coated meshes were easily identified in vivo with APT-MRI during the first 3 weeks postimplantation. The composite meshes magnetization transfer asymmetry ratio (8.7 ± 2.8%) were significantly different from the muscle magnetization transfer asymmetry ratio value (−0.9 ± 1.6%). After a month, the mesh value dropped down to 1.1 ± 3.9%. Muscle and mesh magnetization transfer asymmetry ratio values were not significantly different and mesh conspicuity was no longer possible.


Conclusion
The results suggest that APT-MRI is a promising technique for noninvasive, early postsurgical visualization of composite meshes used in ventral hernia repair. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24663" xmlns="http://purl.org/rss/1.0/"><title>Initial experience with seven tesla magnetic resonance spectroscopy of hypothalamic GABA during hyperinsulinemic euglycemia and hypoglycemia in healthy humans</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24663</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Initial experience with seven tesla magnetic resonance spectroscopy of hypothalamic GABA during hyperinsulinemic euglycemia and hypoglycemia in healthy humans</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. Moheet, U. E. Emir, M. Terpstra, A. Kumar, L. E. Eberly, E. R. Seaquist, G. Öz</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-19T13:10:55.396968-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24663</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24663</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24663</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24663-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Hypothalamic GABA signaling has been shown to regulate the hormonal response to hypoglycemia in animals. The hypothalamus is a challenging brain region for magnetic resonance spectroscopy (MRS) due to its small size and central location. To investigate the feasibility of measuring GABA in the hypothalamus in humans, ultra-high field MRS was used.</p></div></div>
<div class="section" id="mrm24663-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>GABA levels in the hypothalamus and occipital cortex (control region) were measured in healthy volunteers during euglycemia and hypoglycemia at 7 tesla using short-echo STEAM (TE = 8 ms, TR = 5 s).</p></div></div>
<div class="section" id="mrm24663-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Hypothalamic GABA levels were quantified with a mean within-session test–retest coefficient of variance of 9%. Relatively high GABA levels were observed in the hypothalamus compared with other brain regions. Hypothalamic GABA levels were 3.5 ± 0.3 µmol/g during euglycemia (glucose 89 ± 6 mg/dL) vs. 3.0 ± 0.4 µmol/g during hypoglycemia (glucose 61 ± 3 mg/dL) (<em>P</em> = 0.06, <em>N</em> = 7). In the occipital cortex, GABA levels remained constant at 1.4 ± 0.4 vs.1.4 ± 0.3 µmol/g (<em>P</em> = 0.3, <em>N</em> = 5) as glucose fell from 91 ± 4 to 61 ± 4 mg/dL.</p></div></div>
<div class="section" id="mrm24663-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>GABA concentration can be quantified in the human hypothalamus and shows a trend toward decrease in response to an acute fall in blood glucose. These methods can be used to further investigate role of GABA signaling in the counterregulatory response to hypoglycemia in humans. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Hypothalamic GABA signaling has been shown to regulate the hormonal response to hypoglycemia in animals. The hypothalamus is a challenging brain region for magnetic resonance spectroscopy (MRS) due to its small size and central location. To investigate the feasibility of measuring GABA in the hypothalamus in humans, ultra-high field MRS was used.


Methods
GABA levels in the hypothalamus and occipital cortex (control region) were measured in healthy volunteers during euglycemia and hypoglycemia at 7 tesla using short-echo STEAM (TE = 8 ms, TR = 5 s).


Results
Hypothalamic GABA levels were quantified with a mean within-session test–retest coefficient of variance of 9%. Relatively high GABA levels were observed in the hypothalamus compared with other brain regions. Hypothalamic GABA levels were 3.5 ± 0.3 µmol/g during euglycemia (glucose 89 ± 6 mg/dL) vs. 3.0 ± 0.4 µmol/g during hypoglycemia (glucose 61 ± 3 mg/dL) (P = 0.06, N = 7). In the occipital cortex, GABA levels remained constant at 1.4 ± 0.4 vs.1.4 ± 0.3 µmol/g (P = 0.3, N = 5) as glucose fell from 91 ± 4 to 61 ± 4 mg/dL.


Conclusion
GABA concentration can be quantified in the human hypothalamus and shows a trend toward decrease in response to an acute fall in blood glucose. These methods can be used to further investigate role of GABA signaling in the counterregulatory response to hypoglycemia in humans. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24611" xmlns="http://purl.org/rss/1.0/"><title>Myocardial blood flow at rest and stress measured with dynamic contrast-enhanced MRI: Comparison of a distributed parameter model with a fermi function model</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24611</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Myocardial blood flow at rest and stress measured with dynamic contrast-enhanced MRI: Comparison of a distributed parameter model with a fermi function model</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">David A. Broadbent, John D. Biglands, Abdulghani Larghat, Steven P. Sourbron, Aleksandra Radjenovic, John P. Greenwood, Sven Plein, David L. Buckley</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-15T09:55:28.012192-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24611</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24611</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24611</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24611-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To assess the feasibility of simultaneously measuring blood flow (<em>F</em><sub>b</sub>), Gd-DTPA extraction fraction (<em>E</em>), and distribution volume (<em>v</em><sub>d</sub>) in healthy myocardium at rest and under adenosine stress using dynamic contrast-enhanced MRI.</p></div></div>
<div class="section" id="mrm24611-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Sixteen volunteers were examined at 1.5 T and 11 returned for a repeat study. The data were analyzed using a distributed parameter (DP) 2-region model to arrive at estimates of <em>F</em><sub>b</sub>, <em>E</em>, blood volume, and interstitial volume. For comparison, estimates of <em>F</em><sub>b</sub> were also obtained using a Fermi function model.</p></div></div>
<div class="section" id="mrm24611-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>DP model fits were successful in 49 of the 54 data sets. Estimates obtained using DP and Fermi models did not differ for either rest <em>F</em><sub>b</sub> or myocardial perfusion reserve though DP estimates of stress <em>F</em><sub>b</sub> were lower than Fermi estimates. The repeatability of the DP parameters <em>F</em><sub>b</sub>, <em>E</em>, and <em>v</em><sub>d</sub> was better than or equal to the repeatability of Fermi-<em>F</em><sub>b</sub>. <em>E</em> at rest and under stress was estimated to be 66% and 57%, respectively.</p></div></div>
<div class="section" id="mrm24611-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The results suggest that characteristics of the microvasculature of healthy myocardium can be reliably determined using dynamic contrast-enhanced MRI at rest and under stress and that delivery of Gd-DTPA to the myocardium is not flow-limited. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To assess the feasibility of simultaneously measuring blood flow (Fb), Gd-DTPA extraction fraction (E), and distribution volume (vd) in healthy myocardium at rest and under adenosine stress using dynamic contrast-enhanced MRI.


Methods
Sixteen volunteers were examined at 1.5 T and 11 returned for a repeat study. The data were analyzed using a distributed parameter (DP) 2-region model to arrive at estimates of Fb, E, blood volume, and interstitial volume. For comparison, estimates of Fb were also obtained using a Fermi function model.


Results
DP model fits were successful in 49 of the 54 data sets. Estimates obtained using DP and Fermi models did not differ for either rest Fb or myocardial perfusion reserve though DP estimates of stress Fb were lower than Fermi estimates. The repeatability of the DP parameters Fb, E, and vd was better than or equal to the repeatability of Fermi-Fb. E at rest and under stress was estimated to be 66% and 57%, respectively.


Conclusion
The results suggest that characteristics of the microvasculature of healthy myocardium can be reliably determined using dynamic contrast-enhanced MRI at rest and under stress and that delivery of Gd-DTPA to the myocardium is not flow-limited. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24674" xmlns="http://purl.org/rss/1.0/"><title>MR Elastography of the Liver and the Spleen Using a Piezoelectric Driver, Single-Shot Wave-Field Acquisition, and Multifrequency Dual Parameter Reconstruction</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24674</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">MR Elastography of the Liver and the Spleen Using a Piezoelectric Driver, Single-Shot Wave-Field Acquisition, and Multifrequency Dual Parameter Reconstruction</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sebastian Hirsch, Jing Guo, Rolf Reiter, Sebastian Papazoglou, Thomas Kroencke, Juergen Braun, Ingolf Sack</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:16:49.053873-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24674</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24674</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24674</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24674-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Viscoelastic properties of the liver are sensitive to fibrosis. This study proposes several modifications to existing magnetic resonance elastography (MRE) techniques to improve the accuracy of abdominal MRE.</p></div></div>
<div class="section" id="mrm24674-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The proposed method comprises the following steps: (i) wave generation by a nonmagnetic, piezoelectric driver suitable for integration into the patient table, (ii) fast single-shot 3D wave-field acquisition at four drive frequencies between 30 and 60 Hz, and (iii) single-step postprocessing by a novel multifrequency dual parameter inversion of the wave equation. The method is tested in phantoms, healthy volunteers, and patients with portal hypertension and ascites.</p></div></div>
<div class="section" id="mrm24674-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Spatial maps of magnitude and phase of the complex shear modulus were acquired within 6–8 min. These maps are not subject to bias from inversion-related artifacts known from classic MRE. The spatially averaged modulus for healthy liver was 1.44 ± 0.23 kPa with <em>ϕ</em> = 0.492 ± 0.064. Both parameters were significantly higher in the spleen (2.29 ± 0.97 kPa, <em>P</em> = 0.015 and 0.749 ± 0.144, <em>P</em> = 6.58·10<sup>−5</sup>, respectively).</p></div></div>
<div class="section" id="mrm24674-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The proposed method provides abdominal images of viscoelasticity in a short time with spatial resolution comparable to conventional MR images and improved quality without being compromised by ascites. The new setup allows for the integration of abdominal MRE into the clinical workflow. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Viscoelastic properties of the liver are sensitive to fibrosis. This study proposes several modifications to existing magnetic resonance elastography (MRE) techniques to improve the accuracy of abdominal MRE.


Methods
The proposed method comprises the following steps: (i) wave generation by a nonmagnetic, piezoelectric driver suitable for integration into the patient table, (ii) fast single-shot 3D wave-field acquisition at four drive frequencies between 30 and 60 Hz, and (iii) single-step postprocessing by a novel multifrequency dual parameter inversion of the wave equation. The method is tested in phantoms, healthy volunteers, and patients with portal hypertension and ascites.


Results
Spatial maps of magnitude and phase of the complex shear modulus were acquired within 6–8 min. These maps are not subject to bias from inversion-related artifacts known from classic MRE. The spatially averaged modulus for healthy liver was 1.44 ± 0.23 kPa with ϕ = 0.492 ± 0.064. Both parameters were significantly higher in the spleen (2.29 ± 0.97 kPa, P = 0.015 and 0.749 ± 0.144, P = 6.58·10−5, respectively).


Conclusion
The proposed method provides abdominal images of viscoelasticity in a short time with spatial resolution comparable to conventional MR images and improved quality without being compromised by ascites. The new setup allows for the integration of abdominal MRE into the clinical workflow. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24671" xmlns="http://purl.org/rss/1.0/"><title>Thermal Tissue Damage Model Analyzed for Different Whole-Body SAR and Scan Durations for Standard MR Body Coils</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24671</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Thermal Tissue Damage Model Analyzed for Different Whole-Body SAR and Scan Durations for Standard MR Body Coils</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Manuel Murbach, Esra Neufeld, Myles Capstick, Wolfgang Kainz, David O. Brunner, Theodoros Samaras, Klaas P. Pruessmann, Niels Kuster</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:16:38.468041-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24671</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24671</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24671</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24671-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>This article investigates the safety of radiofrequency induced local thermal hotspots within a 1.5T body coil by assessing the transient local peak temperatures as a function of exposure level and local thermoregulation in four anatomical human models in different Z-positions.</p></div></div>
<div class="section" id="mrm24671-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>To quantize the effective thermal stress of the tissues, the thermal dose model cumulative equivalent minutes at 43°C was employed, allowing the prediction of thermal tissue damage risk and the identification of potentially hazardous MR scan-scenarios. The numerical results were validated by B<sub>1</sub><sup>+</sup>− and skin temperature measurements.</p></div></div>
<div class="section" id="mrm24671-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>At continuous 4 W/kg whole-body exposure, peak tissue temperatures of up to 42.8°C were computed for the thermoregulated model (60°C in nonregulated case). When applying cumulative equivalent minutes at 43°C damage thresholds of 15 min (muscle, skin, fat, and bone) and 2 min (other), possible tissue damage cannot be excluded after 25 min for the thermoregulated model (4 min in nonregulated).</p></div></div>
<div class="section" id="mrm24671-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The results are found to be consistent with the history of safe use in MR scanning, but not with current safety guidelines. For future safety concepts, we suggest to use thermal dose models instead of temperatures or SAR. Special safety concerns for patients with impaired thermoregulation (e.g., the elderly, diabetics) should be addressed. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
This article investigates the safety of radiofrequency induced local thermal hotspots within a 1.5T body coil by assessing the transient local peak temperatures as a function of exposure level and local thermoregulation in four anatomical human models in different Z-positions.


Methods
To quantize the effective thermal stress of the tissues, the thermal dose model cumulative equivalent minutes at 43°C was employed, allowing the prediction of thermal tissue damage risk and the identification of potentially hazardous MR scan-scenarios. The numerical results were validated by B1+− and skin temperature measurements.


Results
At continuous 4 W/kg whole-body exposure, peak tissue temperatures of up to 42.8°C were computed for the thermoregulated model (60°C in nonregulated case). When applying cumulative equivalent minutes at 43°C damage thresholds of 15 min (muscle, skin, fat, and bone) and 2 min (other), possible tissue damage cannot be excluded after 25 min for the thermoregulated model (4 min in nonregulated).


Conclusion
The results are found to be consistent with the history of safe use in MR scanning, but not with current safety guidelines. For future safety concepts, we suggest to use thermal dose models instead of temperatures or SAR. Special safety concerns for patients with impaired thermoregulation (e.g., the elderly, diabetics) should be addressed. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24667" xmlns="http://purl.org/rss/1.0/"><title>Volumetric B1+ Mapping of the Brain at 7T using DREAM</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24667</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Volumetric B1+ Mapping of the Brain at 7T using DREAM</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kay Nehrke, Maarten J. Versluis, Andrew Webb, Peter Börnert</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:16:31.731435-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24667</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24667</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24667</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24667-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To tailor and optimize the Dual Refocusing Echo Acquisition Mode (DREAM) approach for volumetric <em>B</em><sub>1</sub><sup>+</sup> mapping of the brain at 7T.</p></div></div>
<div class="section" id="mrm24667-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>A new DREAM echo timing scheme based on the virtual stimulated echo was derived to minimize potential effects of transverse relaxation. Furthermore, the DREAM <em>B</em><sub>1</sub><sup>+</sup> mapping performance was investigated in simulations and experimentally in phantoms and volunteers for volumetric applications, studying and optimizing the accuracy of the sequence with respect to saturation effects, slice profile imperfections, and <em>T</em><sub>1</sub> and <em>T</em><sub>2</sub> relaxation. Volumetric brain protocols were compiled for different isotropic resolutions (5–2.5 mm) and SENSE factors, and were studied in vivo for different RF drive modes (circular/linear polarization) and the application of dielectric pads.</p></div></div>
<div class="section" id="mrm24667-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Volumetric <em>B</em><sub>1</sub><sup>+</sup> maps with good SNR at 2.5 mm isotropic resolution were acquired in about 20 s or less. The specific absorption rate was well below the safety limits for all scans. Mild flow artefacts were observed in the large vessels. Moreover, a slight contrast in the ventricle was observed in the <em>B</em><sub>1</sub><sup>+</sup> maps, which could be attributed to <em>T</em><sub>1</sub> and <em>T</em><sub>2</sub> relaxation effects.</p></div></div>
<div class="section" id="mrm24667-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>DREAM enables safe, very fast, and robust volumetric <em>B</em><sub>1</sub><sup>+</sup> mapping of the brain at ultrahigh fields. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
To tailor and optimize the Dual Refocusing Echo Acquisition Mode (DREAM) approach for volumetric B1+ mapping of the brain at 7T.


Theory and Methods
A new DREAM echo timing scheme based on the virtual stimulated echo was derived to minimize potential effects of transverse relaxation. Furthermore, the DREAM B1+ mapping performance was investigated in simulations and experimentally in phantoms and volunteers for volumetric applications, studying and optimizing the accuracy of the sequence with respect to saturation effects, slice profile imperfections, and T1 and T2 relaxation. Volumetric brain protocols were compiled for different isotropic resolutions (5–2.5 mm) and SENSE factors, and were studied in vivo for different RF drive modes (circular/linear polarization) and the application of dielectric pads.


Results
Volumetric B1+ maps with good SNR at 2.5 mm isotropic resolution were acquired in about 20 s or less. The specific absorption rate was well below the safety limits for all scans. Mild flow artefacts were observed in the large vessels. Moreover, a slight contrast in the ventricle was observed in the B1+ maps, which could be attributed to T1 and T2 relaxation effects.


Conclusion
DREAM enables safe, very fast, and robust volumetric B1+ mapping of the brain at ultrahigh fields. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24665" xmlns="http://purl.org/rss/1.0/"><title>Use of Magnetization Transfer Contrast MRI to Detect Early Molecular Pathology in Alzheimer's Disease</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24665</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Use of Magnetization Transfer Contrast MRI to Detect Early Molecular Pathology in Alzheimer's Disease</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Carlos J. Pérez-Torres, Julia O. Reynolds, Robia G. Pautler</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:16:25.689543-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24665</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24665</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24665</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24665-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The purpose of this study was to determine if magnetization transfer contrast (MTC) imaging could be used to detect early macromolecular accumulation in a mouse model of early Alzheimer's disease.</p></div></div>
<div class="section" id="mrm24665-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>We obtained MTC images at 9.4 T at three different age points in the Tg2576 mouse model of Alzheimer's disease. The Tg2576 mouse exhibits increased amyloid beta deposition that eventually progresses into amyloid beta plaque formation, increased hyper-phosphorylated tau but does not exhibit neurodegeneration.</p></div></div>
<div class="section" id="mrm24665-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Our results show an increase in the MTC signal that predates plaque formation and reported learning and memory deficits in the Tg2576 mouse. This increase in the MTC signal was reversed in a model of antioxidant therapy.</p></div></div>
<div class="section" id="mrm24665-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>MTC magnetic resonance imaging can be used to detect early macromolecular changes in the Tg2576 mouse model of Alzheimer's disease. The source of the MTC contrast is likely complex and warrants further investigation in additional preclinical models that represent early and late stage Alzheimer's disease pathologies. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
The purpose of this study was to determine if magnetization transfer contrast (MTC) imaging could be used to detect early macromolecular accumulation in a mouse model of early Alzheimer's disease.


Methods
We obtained MTC images at 9.4 T at three different age points in the Tg2576 mouse model of Alzheimer's disease. The Tg2576 mouse exhibits increased amyloid beta deposition that eventually progresses into amyloid beta plaque formation, increased hyper-phosphorylated tau but does not exhibit neurodegeneration.


Results
Our results show an increase in the MTC signal that predates plaque formation and reported learning and memory deficits in the Tg2576 mouse. This increase in the MTC signal was reversed in a model of antioxidant therapy.


Conclusion
MTC magnetic resonance imaging can be used to detect early macromolecular changes in the Tg2576 mouse model of Alzheimer's disease. The source of the MTC contrast is likely complex and warrants further investigation in additional preclinical models that represent early and late stage Alzheimer's disease pathologies. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24662" xmlns="http://purl.org/rss/1.0/"><title>Collagen Composition and Content-Dependent Contrast in Porcine Annulus Fibrosus Achieved by Using Double Quantum and Magnetization Transfer Filtered UTE MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24662</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Collagen Composition and Content-Dependent Contrast in Porcine Annulus Fibrosus Achieved by Using Double Quantum and Magnetization Transfer Filtered UTE MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Uzi Eliav, Michal E. Komlosh, Peter J. Basser, Gil Navon</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:16:20.753386-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24662</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24662</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24662</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24662-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To test the potential of combining double quantum and magnetization transfer filtered ultra-short echo time (DQF-MT-UTE) MRI to obtain information about the macromolecular composition and characteristics of connective tissues.</p></div></div>
<div class="section" id="mrm24662-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>A DQF-MT-UTE pulse sequence was implemented on a 14.1 T AVANCE III Bruker spectrometer equipped with a Bruker micro2.5-imaging gradient system to obtain images of porcine annulus fibrosus.</p></div></div>
<div class="section" id="mrm24662-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The DQF-MT-UTE MRI of the annulus fibrosus of porcine intervertebral disc, where the creation time of the double quantum coherence filtering (DQF) was on a time scale appropriate for excitation of macromolecules, showed stronger signal from the outer layers of the disc than from the inner layers closer to the nucleus pulposus. Similarly, spectroscopic studies showed the same trend in the efficiency of the magnetization transfer (MT) from collagen to water.</p></div></div>
<div class="section" id="mrm24662-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>DQF-MT filtered UTE MRI of the annulus fibrosus provides new contrast parameters that depend on the concentration of the collagen and on the rate and efficiency of MT of its protons to water. The latter parameters appear to be different for collagen types I and II in the annulus fibrosus. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
To test the potential of combining double quantum and magnetization transfer filtered ultra-short echo time (DQF-MT-UTE) MRI to obtain information about the macromolecular composition and characteristics of connective tissues.


Methods
A DQF-MT-UTE pulse sequence was implemented on a 14.1 T AVANCE III Bruker spectrometer equipped with a Bruker micro2.5-imaging gradient system to obtain images of porcine annulus fibrosus.


Results
The DQF-MT-UTE MRI of the annulus fibrosus of porcine intervertebral disc, where the creation time of the double quantum coherence filtering (DQF) was on a time scale appropriate for excitation of macromolecules, showed stronger signal from the outer layers of the disc than from the inner layers closer to the nucleus pulposus. Similarly, spectroscopic studies showed the same trend in the efficiency of the magnetization transfer (MT) from collagen to water.


Conclusion
DQF-MT filtered UTE MRI of the annulus fibrosus provides new contrast parameters that depend on the concentration of the collagen and on the rate and efficiency of MT of its protons to water. The latter parameters appear to be different for collagen types I and II in the annulus fibrosus. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24658" xmlns="http://purl.org/rss/1.0/"><title>NMR HRMAS spectroscopy of lung biopsy samples: Comparison study between human, pig, rat, and mouse metabolomics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24658</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">NMR HRMAS spectroscopy of lung biopsy samples: Comparison study between human, pig, rat, and mouse metabolomics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Malika A. Benahmed, Karim Elbayed, François Daubeuf, Nicola Santelmo, Nelly Frossard, Izzie J. Namer</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:13:32.001429-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24658</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24658</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24658</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24658-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Using the metabolomics by NMR high-resolution magic angle spinning spectroscopy, we assessed the lung metabolome of various animal species in order to identify the animal model that could be substituted to human lung in studies on fresh lung biopsies.</p></div></div>
<div class="section" id="mrm24658-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The experiments were conducted on intact lung biopsy samples of pig, rat, mouse, and human using a Bruker Advance III 500 spectrometer. Thirty-five to 39 metabolites were identified and 23 metabolites were quantified. Principal component analysis, partial least-squares discriminant analysis, and analysis of variance tests were performed in order to compare the metabolic profiles of each animal lung biopsies to those of the human lung.</p></div></div>
<div class="section" id="mrm24658-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The metabolic composition between human and pig lung was similar. However, human lung was distinguishable from mouse and rat regarding: Trimethylamine <em>N</em>-oxide and betaïne which were present in rodents but not in human lung, carnitine, and glycerophosphocholine which were present in mouse but not in human lung. Conversely, succinic acid was undetected in rat lung. Furthermore, fatty acids concentration was significantly higher in rodent lungs compared to human lung.</p></div></div>
<div class="section" id="mrm24658-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Using the metabolomics by NMR high-resolution magic angle spinning spectroscopy on lung biopsy, samples allowed to highlight that pig lung seems to be close to human lung as regarding its metabolite composition with more similarities than dissimilarities. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Using the metabolomics by NMR high-resolution magic angle spinning spectroscopy, we assessed the lung metabolome of various animal species in order to identify the animal model that could be substituted to human lung in studies on fresh lung biopsies.


Methods
The experiments were conducted on intact lung biopsy samples of pig, rat, mouse, and human using a Bruker Advance III 500 spectrometer. Thirty-five to 39 metabolites were identified and 23 metabolites were quantified. Principal component analysis, partial least-squares discriminant analysis, and analysis of variance tests were performed in order to compare the metabolic profiles of each animal lung biopsies to those of the human lung.


Results
The metabolic composition between human and pig lung was similar. However, human lung was distinguishable from mouse and rat regarding: Trimethylamine N-oxide and betaïne which were present in rodents but not in human lung, carnitine, and glycerophosphocholine which were present in mouse but not in human lung. Conversely, succinic acid was undetected in rat lung. Furthermore, fatty acids concentration was significantly higher in rodent lungs compared to human lung.


Conclusion
Using the metabolomics by NMR high-resolution magic angle spinning spectroscopy on lung biopsy, samples allowed to highlight that pig lung seems to be close to human lung as regarding its metabolite composition with more similarities than dissimilarities. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24653" xmlns="http://purl.org/rss/1.0/"><title>A fast, analytically based method to optimize local transmit efficiency for a transmit array</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24653</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A fast, analytically based method to optimize local transmit efficiency for a transmit array</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Giuseppe Carluccio, Christopher M. Collins, Danilo Erricolo</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:13:25.950395-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24653</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24653</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24653</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24653-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To develop an analytically based algorithm for rapid optimization of the local radiofrequency magnetic 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24653/asset/equation/mrm24653-math-0002.gif?v=1&amp;t=hh1lk4hs&amp;s=241d63d791ccb2f11ad6096a173a6d17e6cbb1eb" class="inlineGraphic"/> field intensity for a given radiofrequency power through a transmit array. The analytical nature of the method will yield insight to optimization requirements and provides a valuable reference for numerically based searches.</p></div></div>
<div class="section" id="mrm24653-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>With the knowledge of the 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24653/asset/equation/mrm24653-math-0003.gif?v=1&amp;t=hh1lk4ht&amp;s=d4717f500e7e7757d27b9c61775ed2aef2d90b7f" class="inlineGraphic"/> field distribution generated by each single coil of the array, both the phases and the amplitudes of each coil current are optimized to maximize the magnitude of the 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24653/asset/equation/mrm24653-math-0004.gif?v=1&amp;t=hh1lk4hu&amp;s=6c24ef792d92d8bf01a1b4399c3a79204230d6f4" class="inlineGraphic"/> field in a specific location of the body per unit of power transmitted through the array and, consequently, minimizing the whole body specific absorption rate for a given pulse sequence.</p></div></div>
<div class="section" id="mrm24653-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Simulations considering the human body show that the proposed method can reduce the whole-body specific absorption rate for a given 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24653/asset/equation/mrm24653-math-0005.gif?v=1&amp;t=hh1lk4hu&amp;s=a9c3d42bf93428dee94213c0b2fc10497b1209fd" class="inlineGraphic"/> magnitude at the location of interest by a factor of about 6.3 compared to the classic birdcage current configuration, and by a factor of 3.2 compared to phase-only shimming in a case with significant coupling between the elements of the array.</p></div></div>
<div class="section" id="mrm24653-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The proposed method can rapidly provide valuable information pertinent to the optimization of field distributions from transmit arrays. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To develop an analytically based algorithm for rapid optimization of the local radiofrequency magnetic 
(B1+) field intensity for a given radiofrequency power through a transmit array. The analytical nature of the method will yield insight to optimization requirements and provides a valuable reference for numerically based searches.


Methods
With the knowledge of the 
B1+ field distribution generated by each single coil of the array, both the phases and the amplitudes of each coil current are optimized to maximize the magnitude of the 
B1+ field in a specific location of the body per unit of power transmitted through the array and, consequently, minimizing the whole body specific absorption rate for a given pulse sequence.


Results
Simulations considering the human body show that the proposed method can reduce the whole-body specific absorption rate for a given 
B1+ magnitude at the location of interest by a factor of about 6.3 compared to the classic birdcage current configuration, and by a factor of 3.2 compared to phase-only shimming in a case with significant coupling between the elements of the array.


Conclusion
The proposed method can rapidly provide valuable information pertinent to the optimization of field distributions from transmit arrays. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24634" xmlns="http://purl.org/rss/1.0/"><title>Quantitative measurement of cancer metabolism using stimulated echo hyperpolarized carbon-13 MRS</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24634</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Quantitative measurement of cancer metabolism using stimulated echo hyperpolarized carbon-13 MRS</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Christine Leon Swisher, Peder E. Z. Larson, Klaus Kruttwig, Adam B. Kerr, Simon Hu, Robert A. Bok, Andrei Goga, John M. Pauly, Sarah J. Nelson, John Kurhanewicz, Daniel B. Vigneron</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:13:18.79411-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24634</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24634</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24634</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24634-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Magnetic resonance spectroscopy of hyperpolarized substrates allows for the observation of label exchange catalyzed by enzymes providing a powerful tool to investigate tissue metabolism and potentially kinetics in vivo. However, the accuracy of current methods to calculate kinetic parameters has been limited by <em>T</em><sub>1</sub> relaxation effects, extracellular signal contributions, and reduced precision at lower signal-to-noise ratio.</p></div></div>
<div class="section" id="mrm24634-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>To address these challenges, we investigated a new modeling technique using metabolic activity decomposition-stimulated echo acquisition mode. The metabolic activity decomposition-stimulated echo acquisition mode technique separates exchanging from nonexchanging metabolites providing twice the information as conventional techniques.</p></div></div>
<div class="section" id="mrm24634-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>This allowed for accurate measurements of rates of conversion and of multiple <em>T</em><sub>1 </sub>values simultaneously using a single acquisition.</p></div></div>
<div class="section" id="mrm24634-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The additional measurement of <em>T</em><sub>1 </sub>values for the reaction metabolites provides further biological information about the cellular environment of the metabolites. The new technique was investigated through simulations and in vivo studies of transgenic mouse models of cancer demonstrating improved assessments of kinetic rate constants and new T<sub>1 </sub>relaxation value measurements for hyperpolarized <sup>13</sup>C-pyruvate, <sup>13</sup>C-lactate, and <sup>13</sup>C-alanine. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Magnetic resonance spectroscopy of hyperpolarized substrates allows for the observation of label exchange catalyzed by enzymes providing a powerful tool to investigate tissue metabolism and potentially kinetics in vivo. However, the accuracy of current methods to calculate kinetic parameters has been limited by T1 relaxation effects, extracellular signal contributions, and reduced precision at lower signal-to-noise ratio.


Theory and Methods
To address these challenges, we investigated a new modeling technique using metabolic activity decomposition-stimulated echo acquisition mode. The metabolic activity decomposition-stimulated echo acquisition mode technique separates exchanging from nonexchanging metabolites providing twice the information as conventional techniques.


Results
This allowed for accurate measurements of rates of conversion and of multiple T1 values simultaneously using a single acquisition.


Conclusion
The additional measurement of T1 values for the reaction metabolites provides further biological information about the cellular environment of the metabolites. The new technique was investigated through simulations and in vivo studies of transgenic mouse models of cancer demonstrating improved assessments of kinetic rate constants and new T1 relaxation value measurements for hyperpolarized 13C-pyruvate, 13C-lactate, and 13C-alanine. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24613" xmlns="http://purl.org/rss/1.0/"><title>Identification and mitigation of interference sources present in SSB-based wireless MRI receiver arrays</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24613</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Identification and mitigation of interference sources present in SSB-based wireless MRI receiver arrays</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Matthew J. Riffe, Michael D. Twieg, Natalia Gudino, Colin J. Blumenthal, Jeremy A. Heilman, Mark A. Griswold</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:13:06.264008-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24613</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24613</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24613</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24613-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Single sideband amplitude modulation (SSB) is an appealing platform for highly parallel wireless MRI detector arrays because the spacing between channels is ideally limited only by the MRI signal bandwidth. However this assumes that no other sources of interference are present outside that bandwidth. This work investigates the practical interference between multiple SSB-encoded MRI signals.</p></div></div>
<div class="section" id="mrm24613-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Noise from coil preamplifiers and carrier bleed-through are identified as sources of interference. Two different SSB systems were designed for 1.5 T with different noise filtering properties. We show how the differences between the filtered noise profiles impact the received MR signal's dynamic range and image signal-to-noise ratio through simulation, bench measurements, and phantom imaging experiments.</p></div></div>
<div class="section" id="mrm24613-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>When operating individually in the MR scanner, both SSB systems were shown to minimally impact the original DR<sub>sig</sub> and signal-to-noise ratio. Conversely, when all eight channels were operating simultaneously, an average signal-to-noise ratio loss was observed to be 12% in the one system, while a second system with more complex filtering was able to achieve a 3% loss in signal-to-noise ratio.</p></div></div>
<div class="section" id="mrm24613-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Successful wireless transmission of multiple SSB-encoded MRI signals is possible as long as channel interference is properly managed through design and simulation. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Single sideband amplitude modulation (SSB) is an appealing platform for highly parallel wireless MRI detector arrays because the spacing between channels is ideally limited only by the MRI signal bandwidth. However this assumes that no other sources of interference are present outside that bandwidth. This work investigates the practical interference between multiple SSB-encoded MRI signals.


Methods
Noise from coil preamplifiers and carrier bleed-through are identified as sources of interference. Two different SSB systems were designed for 1.5 T with different noise filtering properties. We show how the differences between the filtered noise profiles impact the received MR signal's dynamic range and image signal-to-noise ratio through simulation, bench measurements, and phantom imaging experiments.


Results
When operating individually in the MR scanner, both SSB systems were shown to minimally impact the original DRsig and signal-to-noise ratio. Conversely, when all eight channels were operating simultaneously, an average signal-to-noise ratio loss was observed to be 12% in the one system, while a second system with more complex filtering was able to achieve a 3% loss in signal-to-noise ratio.


Conclusion
Successful wireless transmission of multiple SSB-encoded MRI signals is possible as long as channel interference is properly managed through design and simulation. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24657" xmlns="http://purl.org/rss/1.0/"><title>Fat quantification using multiecho sequences with bipolar gradients: Investigation of accuracy and noise performance</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24657</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Fat quantification using multiecho sequences with bipolar gradients: Investigation of accuracy and noise performance</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Pernilla Peterson, Sven Månsson</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:05:35.531452-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24657</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24657</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24657</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24657-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To investigate the accuracy and noise performance of fat quantification with multiple gradient-echo images acquired using bipolar read-out gradients and compare them with those of the well-established unipolar technique.</p></div></div>
<div class="section" id="mrm24657-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory</h4><div class="para"><p>The bipolar read-out technique induces phase and amplitude errors caused by gradient delays, eddy currents, and frequency-dependent coil sensitivity. In this study, these errors were corrected for jointly with the fat/water separation by modeling the impact of these effects on the signal. This approach did not require acquisition of reference data or modification of the pulse sequence.</p></div></div>
<div class="section" id="mrm24657-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Simulations and a phantom experiment were used to investigate the accuracy and noise performance of the technique and compare them with those of a well-established technique using unipolar read-out gradients. Also, the in vivo feasibility was demonstrated for abdominal applications.</p></div></div>
<div class="section" id="mrm24657-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The phantom experiment demonstrated similar accuracy of the bipolar and unipolar fat quantification techniques. In addition, the noise performance was shown not to be affected by the added estimations of the phase and amplitude errors for most inter-echo times.</p></div></div>
<div class="section" id="mrm24657-sec-0005" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The bipolar technique was found to provide accurate fat quantification with noise performance similar to the unipolar technique given an appropriate choice of inter-echo time. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To investigate the accuracy and noise performance of fat quantification with multiple gradient-echo images acquired using bipolar read-out gradients and compare them with those of the well-established unipolar technique.


Theory
The bipolar read-out technique induces phase and amplitude errors caused by gradient delays, eddy currents, and frequency-dependent coil sensitivity. In this study, these errors were corrected for jointly with the fat/water separation by modeling the impact of these effects on the signal. This approach did not require acquisition of reference data or modification of the pulse sequence.


Methods
Simulations and a phantom experiment were used to investigate the accuracy and noise performance of the technique and compare them with those of a well-established technique using unipolar read-out gradients. Also, the in vivo feasibility was demonstrated for abdominal applications.


Results
The phantom experiment demonstrated similar accuracy of the bipolar and unipolar fat quantification techniques. In addition, the noise performance was shown not to be affected by the added estimations of the phase and amplitude errors for most inter-echo times.


Conclusion
The bipolar technique was found to provide accurate fat quantification with noise performance similar to the unipolar technique given an appropriate choice of inter-echo time. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24641" xmlns="http://purl.org/rss/1.0/"><title>Method for high-resolution imaging of creatine in vivo using chemical exchange saturation transfer</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24641</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Method for high-resolution imaging of creatine in vivo using chemical exchange saturation transfer</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Feliks Kogan, Mohammad Haris, Anup Singh, Kejia Cai, Catherine Debrosse, Ravi Prakash Reddy Nanga, Hari Hariharan, Ravinder Reddy</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:00:59.576853-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24641</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24641</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24641</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24641-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To develop a chemical exchange saturation transfer (CEST)-based technique to measure free creatine (Cr) and to validate the technique by measuring the distribution of Cr in muscle with high spatial resolution before and after exercise.</p></div></div>
<div class="section" id="mrm24641-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Phantom studies were performed to determine contributions from other Cr kinase metabolites to the CEST effect from Cr (CrCEST). CEST, <em>T</em><sub>2</sub>, magnetization transfer ratio and <sup>31</sup>P magnetic resonance spectroscopy acquisitions of the lower leg were performed before and after plantar flexion exercise on a 7T whole-body magnetic resonance scanner on healthy volunteers.</p></div></div>
<div class="section" id="mrm24641-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Phantom studies demonstrated that while Cr exhibited significant CEST effect there were no appreciable contributions from other metabolites. In healthy human subjects, following mild plantar flexion exercise, increases in the CEST effect from Cr were observed, which recovered exponentially back to baseline. This technique exhibited good spatial resolution and was able to differentiate differences in muscle utilization among subjects. The CEST effect from Cr results were compared with <sup>31</sup>P magnetic resonance spectroscopy results showing good agreement in the Cr and phosphocreatine recovery kinetics.</p></div></div>
<div class="section" id="mrm24641-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Demonstrated a CEST-based technique to measure free Cr changes in in vivo muscle. The CEST effect from Cr imaging can spatially map changes in Cr concentration in muscle following mild exercise. This may serve as a tool for the diagnosis and treatment of various disorders affecting muscle. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To develop a chemical exchange saturation transfer (CEST)-based technique to measure free creatine (Cr) and to validate the technique by measuring the distribution of Cr in muscle with high spatial resolution before and after exercise.


Methods
Phantom studies were performed to determine contributions from other Cr kinase metabolites to the CEST effect from Cr (CrCEST). CEST, T2, magnetization transfer ratio and 31P magnetic resonance spectroscopy acquisitions of the lower leg were performed before and after plantar flexion exercise on a 7T whole-body magnetic resonance scanner on healthy volunteers.


Results
Phantom studies demonstrated that while Cr exhibited significant CEST effect there were no appreciable contributions from other metabolites. In healthy human subjects, following mild plantar flexion exercise, increases in the CEST effect from Cr were observed, which recovered exponentially back to baseline. This technique exhibited good spatial resolution and was able to differentiate differences in muscle utilization among subjects. The CEST effect from Cr results were compared with 31P magnetic resonance spectroscopy results showing good agreement in the Cr and phosphocreatine recovery kinetics.


Conclusion
Demonstrated a CEST-based technique to measure free Cr changes in in vivo muscle. The CEST effect from Cr imaging can spatially map changes in Cr concentration in muscle following mild exercise. This may serve as a tool for the diagnosis and treatment of various disorders affecting muscle. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24627" xmlns="http://purl.org/rss/1.0/"><title>In vivo diffusion-weighted MRI using perfluorinated gases: ADC comparison between healthy and elastase-treated rat lungs</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24627</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">In vivo diffusion-weighted MRI using perfluorinated gases: ADC comparison between healthy and elastase-treated rat lungs</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">L. Carrero-González, T. Kaulisch, D. Stiller</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:00:44.393225-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24627</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24627</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24627</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Notes</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24627-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>MRI with perfluorinated gases has been shown as an alternative to hyperpolarized gases to image both microstructure and gas diffusivity in the lung. The aim of this study was to measure diffusion restriction of C<sub>2</sub>F<sub>6</sub> in rat lungs and to compare the different levels of restriction between healthy and emphysematous tissue.</p></div></div>
<div class="section" id="mrm24627-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>For this purpose, two groups of rats—healthy and mono-lobar elastase-induced animals—were measured. While being ventilated with a mixture of C<sub>2</sub>F<sub>6</sub> and oxygen four diffusion weighted 19F-images where acquired for each animal and corresponding ADC-maps were calculated.</p></div></div>
<div class="section" id="mrm24627-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>No significant apparent diffusion coefficient (ADC) differences were found between healthy lungs; however, the elastase treated lungs showed a significant increase in ADC.</p></div></div>
<div class="section" id="mrm24627-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>These results demonstrate that ADC measurements with C<sub>2</sub>F<sub>6</sub> are sensitive to the microstructure of rat lungs showing that the diffusion of this gas is limited to different levels in healthy and in emphysematous tissue. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
MRI with perfluorinated gases has been shown as an alternative to hyperpolarized gases to image both microstructure and gas diffusivity in the lung. The aim of this study was to measure diffusion restriction of C2F6 in rat lungs and to compare the different levels of restriction between healthy and emphysematous tissue.


Methods
For this purpose, two groups of rats—healthy and mono-lobar elastase-induced animals—were measured. While being ventilated with a mixture of C2F6 and oxygen four diffusion weighted 19F-images where acquired for each animal and corresponding ADC-maps were calculated.


Results
No significant apparent diffusion coefficient (ADC) differences were found between healthy lungs; however, the elastase treated lungs showed a significant increase in ADC.


Conclusion
These results demonstrate that ADC measurements with C2F6 are sensitive to the microstructure of rat lungs showing that the diffusion of this gas is limited to different levels in healthy and in emphysematous tissue. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24646" xmlns="http://purl.org/rss/1.0/"><title>Self-navigated tissue phase mapping using a golden-angle spiral acquisition—proof of concept in patients with pulmonary hypertension</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24646</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Self-navigated tissue phase mapping using a golden-angle spiral acquisition—proof of concept in patients with pulmonary hypertension</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jennifer A. Steeden, Daniel S. Knight, Shreya Bali, David Atkinson, Andrew M. Taylor, Vivek Muthurangu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T14:00:40.57419-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24646</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24646</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24646</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24646-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To create a high temporal- and spatial-resolution retrospectively cardiac-gated, tissue phase mapping (TPM) sequence, using an image-based respiratory navigator calculated from the data itself.</p></div></div>
<div class="section" id="mrm24646-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The sequence was based on a golden-angle spiral acquisition. Reconstruction of real-time images allowed creation of an image-based navigator. The expiratory spiral interleaves were then retrospectively cardiac-gated using data binning. TPM data were acquired in 20 healthy volunteers and 10 patients with pulmonary hypertension. Longitudinal and radial myocardial velocities were calculated in the left ventricle and right ventricle.</p></div></div>
<div class="section" id="mrm24646-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The image-based navigator was shown to correlate well with simultaneously acquired airflow data in 10 volunteers(<em>r</em>=0.93±0.04). The TPM navigated images had a significantly higher subjective image quality and edge sharpness (<em>P</em>&lt;0.0001) than averaged spiral TPM. No significant differences in myocardial velocities were seen between conventional Cartesian TPM with navigator respiratory-gating and the proposed self-navigated TPM technique, in 10 volunteers. Significant differences in the velocities were seen between the volunteers and patients in the left ventricle at systole and end diastole and in the right ventricle at end diastole.</p></div></div>
<div class="section" id="mrm24646-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The feasibility of measuring myocardial motion using a golden-angle spiral TPM sequence was demonstrated, with an image-based respiratory navigator calculated from the TPM data itself. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To create a high temporal- and spatial-resolution retrospectively cardiac-gated, tissue phase mapping (TPM) sequence, using an image-based respiratory navigator calculated from the data itself.


Methods
The sequence was based on a golden-angle spiral acquisition. Reconstruction of real-time images allowed creation of an image-based navigator. The expiratory spiral interleaves were then retrospectively cardiac-gated using data binning. TPM data were acquired in 20 healthy volunteers and 10 patients with pulmonary hypertension. Longitudinal and radial myocardial velocities were calculated in the left ventricle and right ventricle.


Results
The image-based navigator was shown to correlate well with simultaneously acquired airflow data in 10 volunteers(r=0.93±0.04). The TPM navigated images had a significantly higher subjective image quality and edge sharpness (P&lt;0.0001) than averaged spiral TPM. No significant differences in myocardial velocities were seen between conventional Cartesian TPM with navigator respiratory-gating and the proposed self-navigated TPM technique, in 10 volunteers. Significant differences in the velocities were seen between the volunteers and patients in the left ventricle at systole and end diastole and in the right ventricle at end diastole.


Conclusion
The feasibility of measuring myocardial motion using a golden-angle spiral TPM sequence was demonstrated, with an image-based respiratory navigator calculated from the TPM data itself. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24660" xmlns="http://purl.org/rss/1.0/"><title>Rapid measurement of arterial input function in mouse tail from projection phases</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24660</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Rapid measurement of arterial input function in mouse tail from projection phases</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jennifer Moroz, Clayton L. Wong, Andrew C. Yung, Piotr Kozlowski, Stefan A. Reinsberg</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-14T13:34:37.087858-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24660</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24660</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24660</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>To measure the arterial input function (AIF) in a mouse tail at high temporal resolution with signal phase of MR projections.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>The technique involves the acquisition of one 2D image before injection, followed by a series of projections before, during, and after contrast injection. Differences in the signal phase, relative to the mean preinjection phase, were calculated and converted into a concentration of Gd.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>An AIF with a temporal resolution of 100 ms was measured and verified with colorimetry (in a flow phantom) and mass spectrometry analysis (in vivo). The projection-based AIF is expected to better represent the rapid contrast kinetics in the blood following injection, thus improving the accuracy of quantitative dynamic contrast-enhanced-MRI analysis. Colorimetry experiments confirmed that signal phase is preferred over magnitude for a precise determination of an AIF. In-vivo experiments demonstrate the feasibility of our approach in mice.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>AIFs can be measured quickly and precisely using phase from projections. Phase data are sensitive to the flow velocity; but this sensitivity is significantly reduced when flow compensation was used. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
To measure the arterial input function (AIF) in a mouse tail at high temporal resolution with signal phase of MR projections.


Methods:
The technique involves the acquisition of one 2D image before injection, followed by a series of projections before, during, and after contrast injection. Differences in the signal phase, relative to the mean preinjection phase, were calculated and converted into a concentration of Gd.


Results:
An AIF with a temporal resolution of 100 ms was measured and verified with colorimetry (in a flow phantom) and mass spectrometry analysis (in vivo). The projection-based AIF is expected to better represent the rapid contrast kinetics in the blood following injection, thus improving the accuracy of quantitative dynamic contrast-enhanced-MRI analysis. Colorimetry experiments confirmed that signal phase is preferred over magnitude for a precise determination of an AIF. In-vivo experiments demonstrate the feasibility of our approach in mice.


Conclusion:
AIFs can be measured quickly and precisely using phase from projections. Phase data are sensitive to the flow velocity; but this sensitivity is significantly reduced when flow compensation was used. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24640" xmlns="http://purl.org/rss/1.0/"><title>Robust reconstruction of B 1+ maps by projection into a spherical functions space</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24640</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Robust reconstruction of B 1+ maps by projection into a spherical functions space</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Alessandro Sbrizzi, Hans Hoogduin, Jan J. Lagendijk, Peter Luijten, Cornelis A. T. van den Berg</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-13T09:13:36.688563-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24640</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24640</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24640</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>Several parallel transmit MRI techniques require knowledge of the transmit radiofrequency field profiles (<em>B</em><span><img alt="math image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24640/asset/equation/tex2gif-stack-3.gif?v=1&amp;s=342e55b99cc7a33a33b5f545ebde9657a4812246" class="inlineGraphic"/></span>). During the past years, various methods have been developed to acquire this information. Often, these methods suffer from long measurement times and produce maps exhibiting regions with poor signal-to-noise ratio and artifacts. In this article, a model-based reconstruction procedure is introduced that improves the robustness of <em>B</em><span><img alt="math image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24640/asset/equation/tex2gif-stack-4.gif?v=1&amp;s=9700c8250c007cdd38df5ed3854cd63fbfedfdc5" class="inlineGraphic"/></span> mapping.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods:</h4><div class="para"><p>The missing information from undersampled <em>B</em><span><img alt="math image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24640/asset/equation/tex2gif-stack-5.gif?v=1&amp;s=3561ff64d42864f20b9aebc2a56a88eab6139af8" class="inlineGraphic"/></span> maps and the regions of poor signal to noise ratio are reconstructed through projection into the space of spherical functions that arise naturally from the solution of the Helmholtz equations in the spherical coordinate system.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>As a result, <em>B</em><span><img alt="math image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24640/asset/equation/tex2gif-stack-6.gif?v=1&amp;s=e9fe33d88c6cc3345d98ed88a142570343c33eea" class="inlineGraphic"/></span> data over a limited range of the field of view/volume is sufficient to reconstruct the <em>B</em><span><img alt="math image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24640/asset/equation/tex2gif-stack-7.gif?v=1&amp;s=a9e58782826b64a083679ade6228ffeddb14e3c3" class="inlineGraphic"/></span> over the full spatial domain in a fast and robust way. The same model is exploited to filter the noise of the measured maps. Results from simulations and in vivo measurements confirm the validity of the proposed method.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>A spherical functions model can well approximate the magnetic fields inside the body with few basis terms. Exploiting this compression capability, <em>B</em><span><img alt="math image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24640/asset/equation/tex2gif-stack-8.gif?v=1&amp;s=9e7b31d7916462dd1da0236f13543083b9a3e9e1" class="inlineGraphic"/></span> maps are reconstructed in regions of unknown or corrupted values. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
Several parallel transmit MRI techniques require knowledge of the transmit radiofrequency field profiles (B 1+). During the past years, various methods have been developed to acquire this information. Often, these methods suffer from long measurement times and produce maps exhibiting regions with poor signal-to-noise ratio and artifacts. In this article, a model-based reconstruction procedure is introduced that improves the robustness of B 1+ mapping.


Theory and Methods:
The missing information from undersampled B 1+ maps and the regions of poor signal to noise ratio are reconstructed through projection into the space of spherical functions that arise naturally from the solution of the Helmholtz equations in the spherical coordinate system.


Results:
As a result, B 1+ data over a limited range of the field of view/volume is sufficient to reconstruct the B 1+ over the full spatial domain in a fast and robust way. The same model is exploited to filter the noise of the measured maps. Results from simulations and in vivo measurements confirm the validity of the proposed method.


Conclusion:
A spherical functions model can well approximate the magnetic fields inside the body with few basis terms. Exploiting this compression capability, B 1+ maps are reconstructed in regions of unknown or corrupted values. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24649" xmlns="http://purl.org/rss/1.0/"><title>Improved intravoxel incoherent motion analysis of diffusion weighted imaging by data driven Bayesian modeling</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24649</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Improved intravoxel incoherent motion analysis of diffusion weighted imaging by data driven Bayesian modeling</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Matthew R. Orton, David J. Collins, Dow-Mu Koh, Martin O. Leach</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-13T09:13:25.213535-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24649</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24649</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24649</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>In addition to the diffusion coefficient, fitting the intravoxel incoherent motion model to multiple b-value diffusion-weighted MR data gives pseudo-diffusion measures associated with rapid signal attenuation at low b-values that are of use in the assessment of a number of pathologies. When summary measures are required, such as the average parameter for a region of interest, least-squares based methods give adequate estimation accuracy. However, using least-squares methods for pixel-wise fitting typically gives noisy estimates, especially for the pseudo-diffusion parameters, which limits the applicability of the approach for assessing spatial features and heterogeneity. In this article, a Bayesian approach using a shrinkage prior model is proposed and is shown to substantially reduce estimation uncertainty so that spatial features in the parameters maps are more clearly apparent. The Bayesian approach has no user-defined parameters, so measures of parameter variation (heterogeneity) over regions of interest are determined by the data alone, whereas it is shown that for the least-squares estimates, measures of variation are essentially determined by user-defined constraints on the parameters. Use of a Bayesian shrinkage prior approach is, therefore, recommended for intravoxel incoherent motion modeling. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div>
]]></content:encoded><description>

In addition to the diffusion coefficient, fitting the intravoxel incoherent motion model to multiple b-value diffusion-weighted MR data gives pseudo-diffusion measures associated with rapid signal attenuation at low b-values that are of use in the assessment of a number of pathologies. When summary measures are required, such as the average parameter for a region of interest, least-squares based methods give adequate estimation accuracy. However, using least-squares methods for pixel-wise fitting typically gives noisy estimates, especially for the pseudo-diffusion parameters, which limits the applicability of the approach for assessing spatial features and heterogeneity. In this article, a Bayesian approach using a shrinkage prior model is proposed and is shown to substantially reduce estimation uncertainty so that spatial features in the parameters maps are more clearly apparent. The Bayesian approach has no user-defined parameters, so measures of parameter variation (heterogeneity) over regions of interest are determined by the data alone, whereas it is shown that for the least-squares estimates, measures of variation are essentially determined by user-defined constraints on the parameters. Use of a Bayesian shrinkage prior approach is, therefore, recommended for intravoxel incoherent motion modeling. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24652" xmlns="http://purl.org/rss/1.0/"><title>Whole-Heart Coronary MRA with 3D Affine Motion Correction Using 3D Image-Based Navigation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24652</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Whole-Heart Coronary MRA with 3D Affine Motion Correction Using 3D Image-Based Navigation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Markus Henningsson, Claudia Prieto, Amedeo Chiribiri, Ghislain Vaillant, Reza Razavi, René M Botnar</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-11T09:55:41.583569-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24652</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24652</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24652</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">000</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24652-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Robust motion correction is necessary to minimize respiratory motion artefacts in coronary MR angiography (CMRA). The state-of-the-art method uses a 1D feet-head translational motion correction approach, and data acquisition is limited to a small window in the respiratory cycle, which prolongs the scan by a factor of 2–3. The purpose of this work was to implement 3D affine motion correction for Cartesian whole-heart CMRA using a 3D navigator (3D-NAV) to allow for data acquisition throughout the whole respiratory cycle.</p></div></div>
<div class="section" id="mrm24652-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>3D affine transformations for different respiratory states (bins) were estimated by using 3D-NAV image acquisitions which were acquired during the startup profiles of a steady-state free precession sequence. The calculated 3D affine transformations were applied to the corresponding high-resolution Cartesian image acquisition which had been similarly binned, to correct for respiratory motion between bins.</p></div></div>
<div class="section" id="mrm24652-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Quantitative and qualitative comparisons showed no statistical difference between images acquired with the proposed method and the reference method using a diaphragmatic navigator with a narrow gating window.</p></div></div>
<div class="section" id="mrm24652-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>We demonstrate that 3D-NAV and 3D affine correction can be used to acquire Cartesian whole-heart 3D coronary artery images with 100% scan efficiency with similar image quality as with the state-of-the-art gated and corrected method with approximately 50% scan efficiency. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Robust motion correction is necessary to minimize respiratory motion artefacts in coronary MR angiography (CMRA). The state-of-the-art method uses a 1D feet-head translational motion correction approach, and data acquisition is limited to a small window in the respiratory cycle, which prolongs the scan by a factor of 2–3. The purpose of this work was to implement 3D affine motion correction for Cartesian whole-heart CMRA using a 3D navigator (3D-NAV) to allow for data acquisition throughout the whole respiratory cycle.


Methods
3D affine transformations for different respiratory states (bins) were estimated by using 3D-NAV image acquisitions which were acquired during the startup profiles of a steady-state free precession sequence. The calculated 3D affine transformations were applied to the corresponding high-resolution Cartesian image acquisition which had been similarly binned, to correct for respiratory motion between bins.


Results
Quantitative and qualitative comparisons showed no statistical difference between images acquired with the proposed method and the reference method using a diaphragmatic navigator with a narrow gating window.


Conclusion
We demonstrate that 3D-NAV and 3D affine correction can be used to acquire Cartesian whole-heart 3D coronary artery images with 100% scan efficiency with similar image quality as with the state-of-the-art gated and corrected method with approximately 50% scan efficiency. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24582" xmlns="http://purl.org/rss/1.0/"><title>Accelerated fractional ventilation imaging with hyperpolarized Gas MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24582</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Accelerated fractional ventilation imaging with hyperpolarized Gas MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kiarash Emami, Yinan Xu, Hooman Hamedani, Harrilla Profka, Stephen Kadlecek, Yi Xin, Masaru Ishii, Rahim R. Rizi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-11T09:55:29.088405-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24582</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24582</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24582</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24582-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To investigate the utility of accelerated imaging to enhance multibreath fractional ventilation (<em>r</em>) measurement accuracy using hyperpolarized gas MRI. Undersampling shortens the breath-hold time, thereby reducing the O<sub>2</sub>-induced signal decay and allows subjects to maintain a more physiologically relevant breathing pattern. Additionally, it may improve <em>r</em> estimation accuracy by reducing radiofrequency destruction of hyperpolarized gas.</p></div></div>
<div class="section" id="mrm24582-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Image acceleration was achieved using an eight-channel phased array coil. Undersampled image acquisition was simulated in a series of ventilation images and data was reconstructed for various matrix sizes (48–128) using generalized auto-calibrating partially parallel acquisition. Parallel accelerated <em>r</em> imaging was also performed on five mechanically ventilated pigs.</p></div></div>
<div class="section" id="mrm24582-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Optimal acceleration factor was fairly invariable (2.0–2.2×) over the range of simulated resolutions. Estimation accuracy progressively improved with higher resolutions (39–51% error reduction). In vivo <em>r</em> values were not significantly different between the two methods: 0.27 ± 0.09, 0.35 ± 0.06, 0.40 ± 0.04 (standard) versus 0.23 ± 0.05, 0.34 ± 0.03, 0.37 ± 0.02 (accelerated); for anterior, medial, and posterior slices, respectively, whereas the corresponding vertical <em>r</em> gradients were significant (<em>P</em> &lt; 0.001): 0.021 ± 0.007 (standard) versus 0.019 ± 0.005 (accelerated) (cm<sup>−1</sup>).</p></div></div>
<div class="section" id="mrm24582-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Quadruple phased array coil simulations resulted in an optimal acceleration factor of ∼2× independent of imaging resolution. Results advocate undersampled image acceleration to improve accuracy of fractional ventilation measurement with hyperpolarized gas MRI. <b>Magn Reson Med, 2013</b>. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To investigate the utility of accelerated imaging to enhance multibreath fractional ventilation (r) measurement accuracy using hyperpolarized gas MRI. Undersampling shortens the breath-hold time, thereby reducing the O2-induced signal decay and allows subjects to maintain a more physiologically relevant breathing pattern. Additionally, it may improve r estimation accuracy by reducing radiofrequency destruction of hyperpolarized gas.


Methods
Image acceleration was achieved using an eight-channel phased array coil. Undersampled image acquisition was simulated in a series of ventilation images and data was reconstructed for various matrix sizes (48–128) using generalized auto-calibrating partially parallel acquisition. Parallel accelerated r imaging was also performed on five mechanically ventilated pigs.


Results
Optimal acceleration factor was fairly invariable (2.0–2.2×) over the range of simulated resolutions. Estimation accuracy progressively improved with higher resolutions (39–51% error reduction). In vivo r values were not significantly different between the two methods: 0.27 ± 0.09, 0.35 ± 0.06, 0.40 ± 0.04 (standard) versus 0.23 ± 0.05, 0.34 ± 0.03, 0.37 ± 0.02 (accelerated); for anterior, medial, and posterior slices, respectively, whereas the corresponding vertical r gradients were significant (P &lt; 0.001): 0.021 ± 0.007 (standard) versus 0.019 ± 0.005 (accelerated) (cm−1).


Conclusion
Quadruple phased array coil simulations resulted in an optimal acceleration factor of ∼2× independent of imaging resolution. Results advocate undersampled image acceleration to improve accuracy of fractional ventilation measurement with hyperpolarized gas MRI. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24615" xmlns="http://purl.org/rss/1.0/"><title>Blind retrospective motion correction of MR images</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24615</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Blind retrospective motion correction of MR images</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Alexander Loktyushin, Hannes Nickisch, Rolf Pohmann, Bernhard Schölkopf</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-11T09:25:05.10778-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24615</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24615</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24615</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>Subject motion can severely degrade MR images. A retrospective motion correction algorithm, Gradient-based motion correction, which significantly reduces ghosting and blurring artifacts due to subject motion was proposed. The technique uses the raw data of standard imaging sequences; no sequence modifications or additional equipment such as tracking devices are required. Rigid motion is assumed.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>The approach iteratively searches for the motion trajectory yielding the sharpest image as measured by the entropy of spatial gradients. The vast space of motion parameters is efficiently explored by gradient-based optimization with a convergence guarantee.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>The method has been evaluated on both synthetic and real data in two and three dimentions using standard imaging techniques. MR images are consistently improved over different kinds of motion trajectories. Using a graphics processing unit implementation, computation times are in the order of a few minutes for a full three-dimentional volume.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>The presented technique can be an alternative or a complement to prospective motion correction methods and is able to improve images with strong motion artifacts from standard imaging sequences without requiring additional data. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
Subject motion can severely degrade MR images. A retrospective motion correction algorithm, Gradient-based motion correction, which significantly reduces ghosting and blurring artifacts due to subject motion was proposed. The technique uses the raw data of standard imaging sequences; no sequence modifications or additional equipment such as tracking devices are required. Rigid motion is assumed.


Methods:
The approach iteratively searches for the motion trajectory yielding the sharpest image as measured by the entropy of spatial gradients. The vast space of motion parameters is efficiently explored by gradient-based optimization with a convergence guarantee.


Results:
The method has been evaluated on both synthetic and real data in two and three dimentions using standard imaging techniques. MR images are consistently improved over different kinds of motion trajectories. Using a graphics processing unit implementation, computation times are in the order of a few minutes for a full three-dimentional volume.


Conclusion:
The presented technique can be an alternative or a complement to prospective motion correction methods and is able to improve images with strong motion artifacts from standard imaging sequences without requiring additional data. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24654" xmlns="http://purl.org/rss/1.0/"><title>Real-Time Multipoint Gastrointestinal 19-Fluorine Catheter Tracking</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24654</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Real-Time Multipoint Gastrointestinal 19-Fluorine Catheter Tracking</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Tobias Hahn, Sebastian Kozerke, Werner Schwizer, Michael Fried, Peter Boesiger, Andreas Steingoetter</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-11T09:24:19.927138-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24654</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24654</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24654</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24654-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To develop MR based real-time gastrointestinal 19-Fluorine (19F) catheter tracking and visualization allowing for real-time detection and feedback of 3D catheter shape and movement as well as catheter-driven adjustments of 1H imaging geometry parameters.</p></div></div>
<div class="section" id="mrm24654-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Data were acquired on a 3T clinical system using 3D Golden Angle radial sampling. Two gastrointestinal catheters incorporating four fiducial 19F markers (65 or 50 µL marker volume) were tracked while being pulled through a gel phantom by an operator inside the MR room with velocities of 2–18 mm/s. During continuous acquisition, k-space profiles were transferred in real-time to an external computer for concurrent reconstruction of 3D 19F images and detection and visualization of marker positions. Based on αthe marker positions, automatic adjustments of 1H imaging planes to facilitate targeted anatomical scanning was implemented.</p></div></div>
<div class="section" id="mrm24654-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Mean tracking reliabilities were 94.5 and 83.6% (catheters 1 and 2) for temporal resolutions 185–740 ms. Reconstruction times of 196 ms were achieved. Real-time visual feedback allowed the operator to accurately control the catheter movement. Catheter-guidance for 1H imaging was reliable.</p></div></div>
<div class="section" id="mrm24654-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The presented real-time 19F MR based framework for the tracking of 19F labeled devices is applicable to combined 19F and 1H MRI guidance of gastrointestinal devices in vivo. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To develop MR based real-time gastrointestinal 19-Fluorine (19F) catheter tracking and visualization allowing for real-time detection and feedback of 3D catheter shape and movement as well as catheter-driven adjustments of 1H imaging geometry parameters.


Methods
Data were acquired on a 3T clinical system using 3D Golden Angle radial sampling. Two gastrointestinal catheters incorporating four fiducial 19F markers (65 or 50 µL marker volume) were tracked while being pulled through a gel phantom by an operator inside the MR room with velocities of 2–18 mm/s. During continuous acquisition, k-space profiles were transferred in real-time to an external computer for concurrent reconstruction of 3D 19F images and detection and visualization of marker positions. Based on αthe marker positions, automatic adjustments of 1H imaging planes to facilitate targeted anatomical scanning was implemented.


Results
Mean tracking reliabilities were 94.5 and 83.6% (catheters 1 and 2) for temporal resolutions 185–740 ms. Reconstruction times of 196 ms were achieved. Real-time visual feedback allowed the operator to accurately control the catheter movement. Catheter-guidance for 1H imaging was reliable.


Conclusion
The presented real-time 19F MR based framework for the tracking of 19F labeled devices is applicable to combined 19F and 1H MRI guidance of gastrointestinal devices in vivo. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24651" xmlns="http://purl.org/rss/1.0/"><title>Positive Contrast MR Imaging of Tendons, Ligaments, and Menisci by Subtraction of Signals From a Double Echo Steady State Sequence (Sub-DESS)</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24651</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Positive Contrast MR Imaging of Tendons, Ligaments, and Menisci by Subtraction of Signals From a Double Echo Steady State Sequence (Sub-DESS)</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Petros Martirosian, Christina Schraml, Fabian Springer, Nina F. Schwenzer, Christian Würslin, Fritz Schick, Michael Deimling</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-11T09:24:02.900827-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24651</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24651</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24651</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24651-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To improve the visualization of fibrous tissues as tendons, ligaments and fibrocartilage structures as menisci by positive contrast using a new 3D Double Echo Steady State (DESS) sequence.</p></div></div>
<div class="section" id="mrm24651-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The proposed 3D DESS sequence works with separate acquisition of a first echo with an echo time (TE<sub>1</sub>) of 1.2 ms followed by a more heavily <em>T</em><sub>2</sub>-weighted second echo recorded at time TE<sub>2</sub>. Subtraction of images from both echoes leads to positive signal from fibrous tissues, whereas in other tissues as musculature and fat the subtraction signal nearly vanishes due to almost similar signal strength in both echoes. Systematic measurements in healthy volunteers with different sets of pulse repetition time (TR), TE<sub>1</sub>, readout bandwidth and flip angle were performed to determine optimal sequence parameters.</p></div></div>
<div class="section" id="mrm24651-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The presented 3D sequence with Cartesian readout requires relatively short measuring time, provides reasonable signal-to-noise ratio and can be easily implemented in protocols for clinical musculoskeletal MR imaging. Degenerative changes or tears of tendons, ligaments and fibrocartilage are known to cause increased water content and therefore prolongation of transverse relaxation times, which leads to reduced signal intensities in the “subtraction images.”</p></div></div>
<div class="section" id="mrm24651-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Positive contrast of fibrous tissue as demonstrated by the proposed sub-DESS approach provides improved conspicuity and allows for three-dimensional reconstruction especially of structures with curved geometry. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
To improve the visualization of fibrous tissues as tendons, ligaments and fibrocartilage structures as menisci by positive contrast using a new 3D Double Echo Steady State (DESS) sequence.


Methods
The proposed 3D DESS sequence works with separate acquisition of a first echo with an echo time (TE1) of 1.2 ms followed by a more heavily T2-weighted second echo recorded at time TE2. Subtraction of images from both echoes leads to positive signal from fibrous tissues, whereas in other tissues as musculature and fat the subtraction signal nearly vanishes due to almost similar signal strength in both echoes. Systematic measurements in healthy volunteers with different sets of pulse repetition time (TR), TE1, readout bandwidth and flip angle were performed to determine optimal sequence parameters.


Results
The presented 3D sequence with Cartesian readout requires relatively short measuring time, provides reasonable signal-to-noise ratio and can be easily implemented in protocols for clinical musculoskeletal MR imaging. Degenerative changes or tears of tendons, ligaments and fibrocartilage are known to cause increased water content and therefore prolongation of transverse relaxation times, which leads to reduced signal intensities in the “subtraction images.”


Conclusion
Positive contrast of fibrous tissue as demonstrated by the proposed sub-DESS approach provides improved conspicuity and allows for three-dimensional reconstruction especially of structures with curved geometry. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24639" xmlns="http://purl.org/rss/1.0/"><title>Sensitivity and Source of Amine-Proton Exchange and Amide-Proton Transfer Magnetic Resonance Imaging in Cerebral Ischemia</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24639</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Sensitivity and Source of Amine-Proton Exchange and Amide-Proton Transfer Magnetic Resonance Imaging in Cerebral Ischemia</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Xiaopeng Zong, Ping Wang, Seong-Gi Kim, Tao Jin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-11T09:23:22.781106-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24639</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24639</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24639</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24639-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Amide-proton transfer (APT) and amine–water proton exchange (APEX) MRI can be viable to map pH-decreasing ischemic regions. However, their exact contributions are unclear.</p></div></div>
<div class="section" id="mrm24639-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>We measured APEX- and APT-weighted magnetization transfer ratio asymmetry (denoted as APEXw and APTw), apparent diffusion coefficient, <em>T</em><sub>2</sub>, and <em>T</em><sub>1</sub> images and localized proton spectra in rats with permanent middle cerebral artery occlusion at 9.4 T. Phantoms and theoretical studies were also performed.</p></div></div>
<div class="section" id="mrm24639-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Within 1-h postocclusion, APEXw and APTw maps showed hyperintensity (3.1% of <em>M</em><sub>0</sub>) and hypointensity (−1.8%), respectively, in regions with decreased apparent diffusion coefficient. Ischemia increased lactate and gamma aminobutyric acid concentrations, but decreased glutamate and taurine concentrations. Over time, the APEXw contrast decreased with glutamate, taurine, and creatine, whereas the APTw contrast and lactate level were similar. Phantom and theoretical studies suggest that the source of APEXw signal is mainly from proteins at normal pH, whereas at decreased pH, gamma aminobutyric acid and glutamate contributions increase, inducing the positive APEXw contrast in ischemic regions. The APTw contrast is sensitive to lactate concentration and pH, but contaminated from contributions of the faster APEX processes.</p></div></div>
<div class="section" id="mrm24639-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Positive APEXw contrast is more sensitive to ischemia than negative APTw contrast. They may provide complementary tissue metabolic information. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Amide-proton transfer (APT) and amine–water proton exchange (APEX) MRI can be viable to map pH-decreasing ischemic regions. However, their exact contributions are unclear.


Methods
We measured APEX- and APT-weighted magnetization transfer ratio asymmetry (denoted as APEXw and APTw), apparent diffusion coefficient, T2, and T1 images and localized proton spectra in rats with permanent middle cerebral artery occlusion at 9.4 T. Phantoms and theoretical studies were also performed.


Results
Within 1-h postocclusion, APEXw and APTw maps showed hyperintensity (3.1% of M0) and hypointensity (−1.8%), respectively, in regions with decreased apparent diffusion coefficient. Ischemia increased lactate and gamma aminobutyric acid concentrations, but decreased glutamate and taurine concentrations. Over time, the APEXw contrast decreased with glutamate, taurine, and creatine, whereas the APTw contrast and lactate level were similar. Phantom and theoretical studies suggest that the source of APEXw signal is mainly from proteins at normal pH, whereas at decreased pH, gamma aminobutyric acid and glutamate contributions increase, inducing the positive APEXw contrast in ischemic regions. The APTw contrast is sensitive to lactate concentration and pH, but contaminated from contributions of the faster APEX processes.


Conclusion
Positive APEXw contrast is more sensitive to ischemia than negative APTw contrast. They may provide complementary tissue metabolic information. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24637" xmlns="http://purl.org/rss/1.0/"><title>Electrical Properties Tomography in the Human Brain at 1.5, 3, and 7T: A Comparison Study</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24637</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Electrical Properties Tomography in the Human Brain at 1.5, 3, and 7T: A Comparison Study</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Astrid L. H. M. W. Lier, Alexander Raaijmakers, Tobias Voigt, Jan J. W. Lagendijk, Peter R. Luijten, Ulrich Katscher, Cornelis A. T. Berg</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-11T09:23:10.730339-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24637</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24637</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24637</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24637-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To investigate the effect of magnetic field strength on the validity of two assumptions (namely, the “transceive phase assumption” and the “phase-only reconstruction”) for electrical properties tomography (EPT) at 1.5, 3, and 7T.</p></div></div>
<div class="section" id="mrm24637-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory</h4><div class="para"><p>Electrical properties tomography is a method to map the conductivity and permittivity using MRI; the <em>B</em><sub>1</sub><em><sup>+</sup></em> amplitude and phase is required as input. The <em>B</em><sub>1</sub><em><sup>+</sup></em> phase, however, cannot be measured and is therefore deduced from the measurable transceive phase using the transceive phase assumption. Also, earlier studies showed that the <em>B</em><sub>1</sub><em><sup>+</sup></em> amplitude is not always required for a reliable conductivity reconstruction; this is the so-called “phase-only conductivity reconstruction.”</p></div></div>
<div class="section" id="mrm24637-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Electromagnetic simulations and MRI measurements of phantoms and the human head.</p></div></div>
<div class="section" id="mrm24637-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Reconstructed conductivity and permittivity maps based on <em>B</em><sub>1</sub><sup>+</sup> distributions at 1.5, 3, and 7T were compared to the expected dielectric properties. The noise level of measurements was also determined.</p></div></div>
<div class="section" id="mrm24637-sec-0005" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The transceive phase assumption is most accurate for low-field strengths and low permittivity and in symmetric objects. The phase-only conductivity reconstruction is only applicable at 1.5 and 3T for the investigated geometries. The measurement precision was found to benefit from a higher field strength, which is related to increased signal-to-noise ratio (SNR) and increased curvature of the <em>B</em><sub>1</sub><sup>+</sup> field. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
To investigate the effect of magnetic field strength on the validity of two assumptions (namely, the “transceive phase assumption” and the “phase-only reconstruction”) for electrical properties tomography (EPT) at 1.5, 3, and 7T.


Theory
Electrical properties tomography is a method to map the conductivity and permittivity using MRI; the B1+ amplitude and phase is required as input. The B1+ phase, however, cannot be measured and is therefore deduced from the measurable transceive phase using the transceive phase assumption. Also, earlier studies showed that the B1+ amplitude is not always required for a reliable conductivity reconstruction; this is the so-called “phase-only conductivity reconstruction.”


Methods
Electromagnetic simulations and MRI measurements of phantoms and the human head.


Results
Reconstructed conductivity and permittivity maps based on B1+ distributions at 1.5, 3, and 7T were compared to the expected dielectric properties. The noise level of measurements was also determined.


Conclusion
The transceive phase assumption is most accurate for low-field strengths and low permittivity and in symmetric objects. The phase-only conductivity reconstruction is only applicable at 1.5 and 3T for the investigated geometries. The measurement precision was found to benefit from a higher field strength, which is related to increased signal-to-noise ratio (SNR) and increased curvature of the B1+ field. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24630" xmlns="http://purl.org/rss/1.0/"><title>Improved slice-selective adiabatic excitation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24630</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Improved slice-selective adiabatic excitation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Priti Balchandani, Gary Glover, John Pauly, Daniel Spielman</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-11T09:21:46.245795-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24630</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24630</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24630</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>The purpose of this work is to design an improved Slice-selective Tunable-flip AdiaBatic Low peak-power Excitation (STABLE) pulse with shorter duration and increased off-resonance immunity to make it suitable for use in a greater range of applications and at higher field strengths. An additional aim is to design a variant of this pulse to achieve <em>B</em><sub>1</sub>-insensitive, fat-suppressed excitation.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>The adiabatic SLR algorithm was used to generate a more uniform spectral pulse envelope for this improved radiofrequency pulse for adiabatic slice-selective excitation, called STABLE-2. Pulse parameters were adjusted to design a version of STABLE-2 with a spectral null centered on lipids.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>In vivo images obtained of the human brain at 3 and 7 T demonstrate that STABLE-2 provides robust, uniform, slice-selective excitation over a range of <em>B</em><sub>1</sub> values. Phantom and in vivo knee images obtained at 3 T demonstrate the effectiveness of STABLE-2 for fat suppression.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions:</h4><div class="para"><p>STABLE-2 achieves <em>B</em><sub>1</sub>-insensitive slice-selective excitation while providing greater off-resonance immunity and a shorter pulse duration, when compared to the original STABLE pulse. In particular, the 9.8-ms STABLE-2 pulse provides slice selectivity over 120 Hz whereas the 21-ms STABLE pulse is limited to 80 Hz off-resonance. <em>B</em><sub>1</sub>-Insensitive fat-suppressed excitation may also be achieved by using a variant of this pulse. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
The purpose of this work is to design an improved Slice-selective Tunable-flip AdiaBatic Low peak-power Excitation (STABLE) pulse with shorter duration and increased off-resonance immunity to make it suitable for use in a greater range of applications and at higher field strengths. An additional aim is to design a variant of this pulse to achieve B1-insensitive, fat-suppressed excitation.


Methods:
The adiabatic SLR algorithm was used to generate a more uniform spectral pulse envelope for this improved radiofrequency pulse for adiabatic slice-selective excitation, called STABLE-2. Pulse parameters were adjusted to design a version of STABLE-2 with a spectral null centered on lipids.


Results:
In vivo images obtained of the human brain at 3 and 7 T demonstrate that STABLE-2 provides robust, uniform, slice-selective excitation over a range of B1 values. Phantom and in vivo knee images obtained at 3 T demonstrate the effectiveness of STABLE-2 for fat suppression.


Conclusions:
STABLE-2 achieves B1-insensitive slice-selective excitation while providing greater off-resonance immunity and a shorter pulse duration, when compared to the original STABLE pulse. In particular, the 9.8-ms STABLE-2 pulse provides slice selectivity over 120 Hz whereas the 21-ms STABLE pulse is limited to 80 Hz off-resonance. B1-Insensitive fat-suppressed excitation may also be achieved by using a variant of this pulse. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24636" xmlns="http://purl.org/rss/1.0/"><title>High-resolution, large dynamic range field map estimation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24636</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High-resolution, large dynamic range field map estimation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Joseph Dagher, Timothy Reese, Ali Bilgin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-11T09:21:17.049075-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24636</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24636</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24636</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>We present a theory and a corresponding method to compute high-resolution field maps over a large dynamic range.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods:</h4><div class="para"><p>We derive a closed-form expression for the error in the field map value when computed from two echoes. We formulate an optimization problem to choose three echo times which result in a pair of maximally distinct error distributions. We use standard field mapping sequences at the prescribed echo times. We then design a corresponding estimation algorithm which takes advantage of the optimized echo times to disambiguate the field offset value.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>We validate our method using high-resolution images of a phantom at 7T. The resulting field maps demonstrate robust mapping over both a large dynamic range, and in low SNR regions. We also present high-resolution offset maps in vivo using both, GRE and multiecho gradient echo sequences. Even though the proposed echo time spacings are larger than the well known phase aliasing cutoff, the resulting field maps exhibit a large dynamic range without the use of phase unwrapping or spatial regularization techniques.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>We demonstrate a novel three-echo field map estimation method which overcomes the traditional noise-dynamic range trade-off. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
We present a theory and a corresponding method to compute high-resolution field maps over a large dynamic range.


Theory and Methods:
We derive a closed-form expression for the error in the field map value when computed from two echoes. We formulate an optimization problem to choose three echo times which result in a pair of maximally distinct error distributions. We use standard field mapping sequences at the prescribed echo times. We then design a corresponding estimation algorithm which takes advantage of the optimized echo times to disambiguate the field offset value.


Results:
We validate our method using high-resolution images of a phantom at 7T. The resulting field maps demonstrate robust mapping over both a large dynamic range, and in low SNR regions. We also present high-resolution offset maps in vivo using both, GRE and multiecho gradient echo sequences. Even though the proposed echo time spacings are larger than the well known phase aliasing cutoff, the resulting field maps exhibit a large dynamic range without the use of phase unwrapping or spatial regularization techniques.


Conclusion:
We demonstrate a novel three-echo field map estimation method which overcomes the traditional noise-dynamic range trade-off. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24642" xmlns="http://purl.org/rss/1.0/"><title>Simultaneous imaging of dual-frequency electrical conductivity using a combination of MREIT and MREPT</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24642</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Simultaneous imaging of dual-frequency electrical conductivity using a combination of MREIT and MREPT</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hyung Joong Kim, Woo Chul Jeong, Saurav Z. K. Sajib, Min-Oh Kim, Oh In Kwon, Eung Je Woo, Dong-Hyun Kim</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-08T06:45:25.34434-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24642</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24642</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24642</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24642-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To propose a single magnetic resonance scan conductivity imaging technique providing dual-frequency characteristics of tissue conductivity.</p></div></div>
<div class="section" id="mrm24642-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Using a modified spin-echo pulse sequence, the magnetic flux density induced by externally injected currents and the 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24642/asset/equation/mrm24642-math-0001.gif?v=1&amp;t=hh1lk4kk&amp;s=829b0880db55dfe6f0617a8a19d330ba66733269" class="inlineGraphic"/> phase map with injected current effects removed were acquired simultaneously. The low-frequency conductivity was reconstructed from the measured magnetic flux density by the projected current density method, while the high-frequency conductivity was reconstructed using the 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24642/asset/equation/mrm24642-math-0002.gif?v=1&amp;t=hh1lk4kk&amp;s=c2cf40848caeadb87e2aa8e0f65c373af4767f32" class="inlineGraphic"/> maps. Three different conductivity phantoms were used to demonstrate low- and high-frequency conductivity characteristics.</p></div></div>
<div class="section" id="mrm24642-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>A conductivity spectrum at two frequencies was successfully acquired with the proposed scheme. Magnetic resonance electrical impedance tomography is advantageous for seeing an anomaly itself wrapped with a thin insulating membrane. In addition, if the membrane is porous, the membrane property can be quantitatively visualized with magnetic resonance electrical impedance tomography. Magnetic resonance electrical properties tomography does not detect such membranes, which enable it to probe things inside an insulating membrane.</p></div></div>
<div class="section" id="mrm24642-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Considering these pros and cons and also the fact that the conductivity of biological tissue changes with frequency, a dual-frequency conductivity imaging incorporating both magnetic resonance electrical impedance tomography and magnetic resonance electrical properties tomography in future animal and human experiments is suggested.</p></div></div>
]]></content:encoded><description>

Purpose
To propose a single magnetic resonance scan conductivity imaging technique providing dual-frequency characteristics of tissue conductivity.


Methods
Using a modified spin-echo pulse sequence, the magnetic flux density induced by externally injected currents and the 
B1+ phase map with injected current effects removed were acquired simultaneously. The low-frequency conductivity was reconstructed from the measured magnetic flux density by the projected current density method, while the high-frequency conductivity was reconstructed using the 
B1+ maps. Three different conductivity phantoms were used to demonstrate low- and high-frequency conductivity characteristics.


Results
A conductivity spectrum at two frequencies was successfully acquired with the proposed scheme. Magnetic resonance electrical impedance tomography is advantageous for seeing an anomaly itself wrapped with a thin insulating membrane. In addition, if the membrane is porous, the membrane property can be quantitatively visualized with magnetic resonance electrical impedance tomography. Magnetic resonance electrical properties tomography does not detect such membranes, which enable it to probe things inside an insulating membrane.


Conclusion
Considering these pros and cons and also the fact that the conductivity of biological tissue changes with frequency, a dual-frequency conductivity imaging incorporating both magnetic resonance electrical impedance tomography and magnetic resonance electrical properties tomography in future animal and human experiments is suggested.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24597" xmlns="http://purl.org/rss/1.0/"><title>MRI analysis of cerebellar and vestibular developmental phenotypes in Gbx2 conditional knockout mice</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24597</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">MRI analysis of cerebellar and vestibular developmental phenotypes in Gbx2 conditional knockout mice</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kamila U. Szulc, Brian J. Nieman, Edward J. Houston, Benjamin B. Bartelle, Jason P. Lerch, Alexandra L. Joyner, Daniel H. Turnbull</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-07T17:08:51.724862-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24597</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24597</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24597</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24597-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Our aim in this study was to apply three-dimensional MRI methods to analyze early postnatal morphological phenotypes in a <em>Gbx2</em> conditional knockout (<em>Gbx2-</em>CKO) mouse that has variable midline deletions in the central cerebellum, reminiscent of many human cerebellar hypoplasia syndromes.</p></div></div>
<div class="section" id="mrm24597-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>In vivo three-dimensional manganese-enhanced MRI at 100-µm isotropic resolution was used to visualize mouse brains between postnatal days 3 and 11, when cerebellum morphology undergoes dramatic changes. Deformation-based morphometry and volumetric analysis of manganese-enhanced MRI images were used to, respectively, detect and quantify morphological phenotypes in <em>Gbx2</em>-CKO mice. Ex vivo micro-MRI was performed after perfusion-fixation with supplemented gadolinium for higher resolution (50-µm) analysis.</p></div></div>
<div class="section" id="mrm24597-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>In vivo manganese-enhanced MRI and deformation-based morphometry correctly identified known cerebellar defects in <em>Gbx2-</em>CKO mice, and novel phenotypes were discovered in the deep cerebellar nuclei and the vestibulo-cerebellum, both validated using histology. Ex vivo micro-MRI revealed subtle phenotypes in both the vestibulo-cerebellum and the vestibulo-cochlear organ, providing an interesting example of complementary phenotypes in a sensory organ and its associated brain region.</p></div></div>
<div class="section" id="mrm24597-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>These results show the potential of three-dimensional MRI for detecting and analyzing developmental defects in mouse models of neurodevelopmental diseases. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Our aim in this study was to apply three-dimensional MRI methods to analyze early postnatal morphological phenotypes in a Gbx2 conditional knockout (Gbx2-CKO) mouse that has variable midline deletions in the central cerebellum, reminiscent of many human cerebellar hypoplasia syndromes.


Methods
In vivo three-dimensional manganese-enhanced MRI at 100-µm isotropic resolution was used to visualize mouse brains between postnatal days 3 and 11, when cerebellum morphology undergoes dramatic changes. Deformation-based morphometry and volumetric analysis of manganese-enhanced MRI images were used to, respectively, detect and quantify morphological phenotypes in Gbx2-CKO mice. Ex vivo micro-MRI was performed after perfusion-fixation with supplemented gadolinium for higher resolution (50-µm) analysis.


Results
In vivo manganese-enhanced MRI and deformation-based morphometry correctly identified known cerebellar defects in Gbx2-CKO mice, and novel phenotypes were discovered in the deep cerebellar nuclei and the vestibulo-cerebellum, both validated using histology. Ex vivo micro-MRI revealed subtle phenotypes in both the vestibulo-cerebellum and the vestibulo-cochlear organ, providing an interesting example of complementary phenotypes in a sensory organ and its associated brain region.


Conclusion
These results show the potential of three-dimensional MRI for detecting and analyzing developmental defects in mouse models of neurodevelopmental diseases. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24623" xmlns="http://purl.org/rss/1.0/"><title>Effects of image reconstruction on fibre orientation mapping from multichannel diffusion MRI: Reducing the noise floor using SENSE</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24623</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Effects of image reconstruction on fibre orientation mapping from multichannel diffusion MRI: Reducing the noise floor using SENSE</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">S. N. Sotiropoulos, S. Moeller, S. Jbabdi, J. Xu, J. L. Andersson, E. J. Auerbach, E. Yacoub, D. Feinberg, K. Setsompop, L. L. Wald, T. E. J. Behrens, K. Ugurbil, C. Lenglet</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-07T13:58:33.192673-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24623</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24623</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24623</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24623-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To examine the effects of the reconstruction algorithm of magnitude images from multichannel diffusion MRI on fibre orientation estimation.</p></div></div>
<div class="section" id="mrm24623-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>It is well established that the method used to combine signals from different coil elements in multichannel MRI can have an impact on the properties of the reconstructed magnitude image. Using a root-sum-of-squares approach results in a magnitude signal that follows an effective noncentral-χ distribution. As a result, the noise floor, the minimum measurable in the absence of any true signal, is elevated. This is particularly relevant for diffusion-weighted MRI, where the signal attenuation is of interest.</p></div></div>
<div class="section" id="mrm24623-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>In this study, we illustrate problems that such image reconstruction characteristics may cause in the estimation of fibre orientations, both for model-based and model-free approaches, when modern 32-channel coils are used. We further propose an alternative image reconstruction method that is based on sensitivity encoding (SENSE) and preserves the Rician nature of the single-channel, magnitude MR signal. We show that for the same k-space data, root-sum-of-squares can cause excessive overfitting and reduced precision in orientation estimation compared with the SENSE-based approach.</p></div></div>
<div class="section" id="mrm24623-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>These results highlight the importance of choosing the appropriate image reconstruction method for tractography studies that use multichannel receiver coils for diffusion MRI acquisition. Magn Reson Med, 2013. ©2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To examine the effects of the reconstruction algorithm of magnitude images from multichannel diffusion MRI on fibre orientation estimation.


Theory and Methods
It is well established that the method used to combine signals from different coil elements in multichannel MRI can have an impact on the properties of the reconstructed magnitude image. Using a root-sum-of-squares approach results in a magnitude signal that follows an effective noncentral-χ distribution. As a result, the noise floor, the minimum measurable in the absence of any true signal, is elevated. This is particularly relevant for diffusion-weighted MRI, where the signal attenuation is of interest.


Results
In this study, we illustrate problems that such image reconstruction characteristics may cause in the estimation of fibre orientations, both for model-based and model-free approaches, when modern 32-channel coils are used. We further propose an alternative image reconstruction method that is based on sensitivity encoding (SENSE) and preserves the Rician nature of the single-channel, magnitude MR signal. We show that for the same k-space data, root-sum-of-squares can cause excessive overfitting and reduced precision in orientation estimation compared with the SENSE-based approach.


Conclusion
These results highlight the importance of choosing the appropriate image reconstruction method for tractography studies that use multichannel receiver coils for diffusion MRI acquisition. Magn Reson Med, 2013. ©2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24599" xmlns="http://purl.org/rss/1.0/"><title>Efficient Bloch-Siegert B1+ mapping using spiral and echo-planar readouts</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24599</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Efficient Bloch-Siegert B1+ mapping using spiral and echo-planar readouts</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Manojkumar Saranathan, Mohammad Mehdi Khalighi, Gary H. Glover, Prachi Pandit, Brian K. Rutt</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-07T13:58:07.823744-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24599</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24599</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24599</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The Bloch-Siegert (B-S) <em>B</em><sub>1</sub><sup>+</sup> mapping technique is a fast, phase-based method that is highly SAR limited especially at 7T, necessitating the use of long repetition times. Spiral and echo-planar readouts were incorporated in a gradient-echo based B-S sequence to reduce specific absoprtion rate (SAR) and improve its scan efficiency. A novel, numerically optimized 4 ms B-S off-resonant pulse at + 1960 Hz was used to increase sensitivity and further reduce SAR compared with the conventional 6 ms Fermi B-S pulse. Using echo-planar and spiral readouts, scan time reductions of 8–16 were achieved. By reducing the B-S pulse width by a factor of 1.5, SAR was reduced by a factor of 1.5 and overall sensitivity was increased by a factor of 1.33 due to the nearly halved resonance offset of the new B-S pulse. This was validated on phantoms and volunteers at 7 T. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div>
]]></content:encoded><description>
The Bloch-Siegert (B-S) B1+ mapping technique is a fast, phase-based method that is highly SAR limited especially at 7T, necessitating the use of long repetition times. Spiral and echo-planar readouts were incorporated in a gradient-echo based B-S sequence to reduce specific absoprtion rate (SAR) and improve its scan efficiency. A novel, numerically optimized 4 ms B-S off-resonant pulse at + 1960 Hz was used to increase sensitivity and further reduce SAR compared with the conventional 6 ms Fermi B-S pulse. Using echo-planar and spiral readouts, scan time reductions of 8–16 were achieved. By reducing the B-S pulse width by a factor of 1.5, SAR was reduced by a factor of 1.5 and overall sensitivity was increased by a factor of 1.33 due to the nearly halved resonance offset of the new B-S pulse. This was validated on phantoms and volunteers at 7 T. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24608" xmlns="http://purl.org/rss/1.0/"><title>Novel retrospective, respiratory-gating method enables 3D, high resolution, dynamic imaging of the upper airway during tidal breathing</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24608</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Novel retrospective, respiratory-gating method enables 3D, high resolution, dynamic imaging of the upper airway during tidal breathing</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mark E. Wagshul, Sanghun Sin, Michael L. Lipton, Keivan Shifteh, Raanan Arens</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-07T13:57:43.552793-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24608</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24608</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24608</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24608-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>A retrospective, respiratory-gated technique for measuring dynamic changes in the upper airway over the respiratory cycle was developed, with the ultimate goal of constructing anatomically and functionally accurate upper airway models in obstructive sleep apnea patients.</p></div></div>
<div class="section" id="mrm24608-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Three-dimensional cine, retrospective respiratory-gated, gradient echo imaging was performed in six adolescents being evaluated for polycystic ovary syndrome, a disorder with a high obstructive sleep apnea prevalence. A novel retrospective gating scheme, synchronized to flow from a nasal cannula, limited image acquisition to predefined physiological ranges. Images were evaluated with respect to contrast, airway signal leakage, and demonstration of dynamic airway area changes.</p></div></div>
<div class="section" id="mrm24608-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Two patients were diagnosed with obstructive sleep apnea. Motion artifacts were absent in all image sets. Scan efficiency ranged from 48 to 88%. Soft tissue-to-airway contrast-to-noise ratio varied from 6.1 to 9.6. Airway signal leakage varied between 10 and 17% of soft tissue signal. Automated segmentation allowed calculation of airway area changes over the respiratory cycle. In one severe apnea patient, the technique allowed demonstration of asynchronous airway expansion and contraction above and below a severe constriction.</p></div></div>
<div class="section" id="mrm24608-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>Retrospective, respiratory gated imaging of the upper airway has been demonstrated, utilizing a gating algorithm to ensure acquisition over specified ranges of respiratory rate and tidal volume. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
A retrospective, respiratory-gated technique for measuring dynamic changes in the upper airway over the respiratory cycle was developed, with the ultimate goal of constructing anatomically and functionally accurate upper airway models in obstructive sleep apnea patients.


Methods
Three-dimensional cine, retrospective respiratory-gated, gradient echo imaging was performed in six adolescents being evaluated for polycystic ovary syndrome, a disorder with a high obstructive sleep apnea prevalence. A novel retrospective gating scheme, synchronized to flow from a nasal cannula, limited image acquisition to predefined physiological ranges. Images were evaluated with respect to contrast, airway signal leakage, and demonstration of dynamic airway area changes.


Results
Two patients were diagnosed with obstructive sleep apnea. Motion artifacts were absent in all image sets. Scan efficiency ranged from 48 to 88%. Soft tissue-to-airway contrast-to-noise ratio varied from 6.1 to 9.6. Airway signal leakage varied between 10 and 17% of soft tissue signal. Automated segmentation allowed calculation of airway area changes over the respiratory cycle. In one severe apnea patient, the technique allowed demonstration of asynchronous airway expansion and contraction above and below a severe constriction.


Conclusions
Retrospective, respiratory gated imaging of the upper airway has been demonstrated, utilizing a gating algorithm to ensure acquisition over specified ranges of respiratory rate and tidal volume. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24622" xmlns="http://purl.org/rss/1.0/"><title>Induced clustered nanoconfinement of superparamagnetic iron oxide in biodegradable nanoparticles enhances transverse relaxivity for targeted theranostics</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24622</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Induced clustered nanoconfinement of superparamagnetic iron oxide in biodegradable nanoparticles enhances transverse relaxivity for targeted theranostics</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Ragy R. T. Ragheb, Dongin Kim, Arunima Bandyopadhyay, Halima Chahboune, Beyza Bulutoglu, Harib Ezaldein, Jason M. Criscione, Tarek M. Fahmy</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-07T13:56:53.631775-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24622</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24622</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24622</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24622-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Combined therapeutic and diagnostic agents, “theranostics” are emerging valuable tools for noninvasive imaging and drug delivery. Here, we report on a solid biodegradable multifunctional nanoparticle that combines both features.</p></div></div>
<div class="section" id="mrm24622-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Poly(lactide-<em>co</em>-glycolide) nanoparticles were engineered to confine superparamagnetic iron oxide contrast for magnetic resonance imaging while enabling controlled drug delivery and targeting to specific cells. To achieve this dual modality, fatty acids were used as anchors for surface ligands and for encapsulated iron oxide in the polymer matrix.</p></div></div>
<div class="section" id="mrm24622-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>We demonstrate that fatty acid modified iron oxide prolonged retention of the contrast agent in the polymer matrix during degradative release of drug. Antibody-fatty acid surface modification facilitated cellular targeting and subsequent internalization in cells while inducing clustering of encapsulated fatty-acid modified superparamagnetic iron oxide during particle formulation. This induced clustered confinement led to an aggregation within the nanoparticle and, hence, higher transverse relaxivity, <em>r</em><sub>2</sub>, (294 mM<sup>−1</sup> s<sup>−1</sup>) compared with nanoparticles without fatty-acid ligands (160 mM<sup>−1</sup> s<sup>−1</sup>) and higher than commercially available superparamagnetic iron oxide nanoparticles (89 mM<sup>−1</sup> s<sup>−1</sup>).</p></div></div>
<div class="section" id="mrm24622-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Clustering of superparamagnetic iron oxide in poly(lactide-<em>co</em>-glycolide) did not affect the controlled release of encapsulated drugs such as methotrexate or clodronate and their subsequent pharmacological activity, thus highlighting the full theranostic capability of our system. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Combined therapeutic and diagnostic agents, “theranostics” are emerging valuable tools for noninvasive imaging and drug delivery. Here, we report on a solid biodegradable multifunctional nanoparticle that combines both features.


Methods
Poly(lactide-co-glycolide) nanoparticles were engineered to confine superparamagnetic iron oxide contrast for magnetic resonance imaging while enabling controlled drug delivery and targeting to specific cells. To achieve this dual modality, fatty acids were used as anchors for surface ligands and for encapsulated iron oxide in the polymer matrix.


Results
We demonstrate that fatty acid modified iron oxide prolonged retention of the contrast agent in the polymer matrix during degradative release of drug. Antibody-fatty acid surface modification facilitated cellular targeting and subsequent internalization in cells while inducing clustering of encapsulated fatty-acid modified superparamagnetic iron oxide during particle formulation. This induced clustered confinement led to an aggregation within the nanoparticle and, hence, higher transverse relaxivity, r2, (294 mM−1 s−1) compared with nanoparticles without fatty-acid ligands (160 mM−1 s−1) and higher than commercially available superparamagnetic iron oxide nanoparticles (89 mM−1 s−1).


Conclusion
Clustering of superparamagnetic iron oxide in poly(lactide-co-glycolide) did not affect the controlled release of encapsulated drugs such as methotrexate or clodronate and their subsequent pharmacological activity, thus highlighting the full theranostic capability of our system. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24628" xmlns="http://purl.org/rss/1.0/"><title>Whole-heart coronary MRA with 100% respiratory gating efficiency: Self-navigated three-dimensional retrospective image-based motion correction (TRIM)</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24628</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Whole-heart coronary MRA with 100% respiratory gating efficiency: Self-navigated three-dimensional retrospective image-based motion correction (TRIM)</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jianing Pang, Himanshu Bhat, Behzad Sharif, Zhaoyang Fan, Louise E. J. Thomson, Troy LaBounty, John D. Friedman, James Min, Daniel S. Berman, Debiao Li</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-07T13:56:26.41502-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24628</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24628</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24628</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24628-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To develop a three-dimensional retrospective image-based motion correction technique for whole-heart coronary MRA with self-navigation that eliminates both the need to setup a diaphragm navigator and gate the acquisition.</p></div></div>
<div class="section" id="mrm24628-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The proposed technique uses one-dimensional self-navigation to track the superior–inferior translation of the heart, with which the acquired three-dimensional radial k-space data is segmented into different respiratory bins. Respiratory motion is then estimated in image space using an affine transform model and subsequently this information is used to perform efficient motion correction in k-space. The performance of the proposed technique on healthy volunteers is compared with the conventional navigator gating approach as well as data binning using diaphragm navigator.</p></div></div>
<div class="section" id="mrm24628-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The proposed method is able to reduce the imaging time to 7.1±0.5 min from 13.9±2.6 min with conventional navigator gating. The scan setup time is reduced as well due to the elimination of the navigator. The proposed method yields excellent image quality comparable with either conventional navigator gating or the navigator binning approach.</p></div></div>
<div class="section" id="mrm24628-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>We have developed a new respiratory motion correction technique for coronary MRA that enables 1 mm<sup>3</sup> isotropic resolution and whole-heart coverage with 7 min of scan time. Further tests on patient population are needed to determine its clinical usage. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To develop a three-dimensional retrospective image-based motion correction technique for whole-heart coronary MRA with self-navigation that eliminates both the need to setup a diaphragm navigator and gate the acquisition.


Methods
The proposed technique uses one-dimensional self-navigation to track the superior–inferior translation of the heart, with which the acquired three-dimensional radial k-space data is segmented into different respiratory bins. Respiratory motion is then estimated in image space using an affine transform model and subsequently this information is used to perform efficient motion correction in k-space. The performance of the proposed technique on healthy volunteers is compared with the conventional navigator gating approach as well as data binning using diaphragm navigator.


Results
The proposed method is able to reduce the imaging time to 7.1±0.5 min from 13.9±2.6 min with conventional navigator gating. The scan setup time is reduced as well due to the elimination of the navigator. The proposed method yields excellent image quality comparable with either conventional navigator gating or the navigator binning approach.


Conclusion
We have developed a new respiratory motion correction technique for coronary MRA that enables 1 mm3 isotropic resolution and whole-heart coverage with 7 min of scan time. Further tests on patient population are needed to determine its clinical usage. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24631" xmlns="http://purl.org/rss/1.0/"><title>Principal component analysis enhances SNR for dynamic electron paramagnetic resonance oxygen imaging of cycling hypoxia in vivo</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24631</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Principal component analysis enhances SNR for dynamic electron paramagnetic resonance oxygen imaging of cycling hypoxia in vivo</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Gage Redler, Boris Epel, Howard J. Halpern</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-07T13:56:03.721725-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24631</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24631</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24631</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24631-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Low oxygen concentration (hypoxia) in tumors strongly affects their malignant state and resistance to therapy. These effects may be more deleterious in regions undergoing cycling hypoxia. Electron paramagnetic resonance imaging (EPRI) has provided a noninvasive, quantitative imaging modality to investigate static pO<sub>2</sub> in vivo. However, to image changing hypoxia, EPRI images with better temporal resolution may be required. The tradeoff between temporal resolution and signal-to-noise ratio (SNR) results in lower SNR for EPRI images with imaging time short enough to resolve cycling hypoxia.</p></div></div>
<div class="section" id="mrm24631-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Principal component analysis allows for accelerated image acquisition with acceptable SNR by filtering noise in projection data, from which pO<sub>2</sub> images are reconstructed. Principal component analysis is used as a denoising technique by including only low-order components to approximate the EPRI projection data.</p></div></div>
<div class="section" id="mrm24631-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Simulated and experimental studies show that principal component analysis filtering increases SNR, particularly for small numbers of sub-volumes with changing pO<sub>2</sub>, enabling an order of magnitude increase in temporal resolution with minimal deterioration in spatial resolution or image quality.</p></div></div>
<div class="section" id="mrm24631-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The SNR necessary for dynamic EPRI studies with temporal resolution required to investigate cycling hypoxia and its physiological implications is enabled by principal component analysis filtering. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Low oxygen concentration (hypoxia) in tumors strongly affects their malignant state and resistance to therapy. These effects may be more deleterious in regions undergoing cycling hypoxia. Electron paramagnetic resonance imaging (EPRI) has provided a noninvasive, quantitative imaging modality to investigate static pO2 in vivo. However, to image changing hypoxia, EPRI images with better temporal resolution may be required. The tradeoff between temporal resolution and signal-to-noise ratio (SNR) results in lower SNR for EPRI images with imaging time short enough to resolve cycling hypoxia.


Methods
Principal component analysis allows for accelerated image acquisition with acceptable SNR by filtering noise in projection data, from which pO2 images are reconstructed. Principal component analysis is used as a denoising technique by including only low-order components to approximate the EPRI projection data.


Results
Simulated and experimental studies show that principal component analysis filtering increases SNR, particularly for small numbers of sub-volumes with changing pO2, enabling an order of magnitude increase in temporal resolution with minimal deterioration in spatial resolution or image quality.


Conclusion
The SNR necessary for dynamic EPRI studies with temporal resolution required to investigate cycling hypoxia and its physiological implications is enabled by principal component analysis filtering. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24648" xmlns="http://purl.org/rss/1.0/"><title>Water/fat-resolved whole-heart Dixon coronary MRA: An initial comparison</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24648</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Water/fat-resolved whole-heart Dixon coronary MRA: An initial comparison</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Peter Börnert, Peter Koken, Kay Nehrke, Holger Eggers, Peter Ostendorf</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-07T13:53:11.904643-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24648</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24648</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24648</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24648-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To improve coronary vessel visualization in whole-heart coronary magnetic resonance angiography (CMRA), fat suppression is typically applied. However, recent studies have shown that cardiac fat can also have diagnostic value. To enhance CMRA image quality by improved fat suppression and to provide additionally fat-only information highly resolved, dual-echo Dixon CMRA approaches have been developed.</p></div></div>
<div class="section" id="mrm24648-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>In this pilot study, approved by the institutional review board, 30 patients were investigated comparing whole-heart T<sub>1</sub>-weighted dual-echo Dixon CMRA to conventional whole-heart fat-suppressed balanced fast field echo CMRA, integrated into a routine clinical protocol that includes the administration of gadolinium for perfusion and late enhancement measurements. Signal-to-noise-ratio, contrast-to-noise-ratio, and image quality were analyzed.</p></div></div>
<div class="section" id="mrm24648-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Dual-echo Dixon significantly (<em>P</em>&lt;0.000001) improved image quality compared with conventional fat-suppressed balanced fast field echo CMRA. Signal-to-noise-ratio and contrast-to-noise-ratio were found to be comparable when balanced fast field echo was performed before gadolinium and dual-echo Dixon fast field echo after gadolinium administration.</p></div></div>
<div class="section" id="mrm24648-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Dual-echo Dixon can help to improve whole-heart CMRA image quality significantly. The additional whole-heart fat information delivered by this approach can support a number of new clinical studies addressing the diagnostic and the predictive value of intramyocardial and extramyocardial fatty deposits. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To improve coronary vessel visualization in whole-heart coronary magnetic resonance angiography (CMRA), fat suppression is typically applied. However, recent studies have shown that cardiac fat can also have diagnostic value. To enhance CMRA image quality by improved fat suppression and to provide additionally fat-only information highly resolved, dual-echo Dixon CMRA approaches have been developed.


Methods
In this pilot study, approved by the institutional review board, 30 patients were investigated comparing whole-heart T1-weighted dual-echo Dixon CMRA to conventional whole-heart fat-suppressed balanced fast field echo CMRA, integrated into a routine clinical protocol that includes the administration of gadolinium for perfusion and late enhancement measurements. Signal-to-noise-ratio, contrast-to-noise-ratio, and image quality were analyzed.


Results
Dual-echo Dixon significantly (P&lt;0.000001) improved image quality compared with conventional fat-suppressed balanced fast field echo CMRA. Signal-to-noise-ratio and contrast-to-noise-ratio were found to be comparable when balanced fast field echo was performed before gadolinium and dual-echo Dixon fast field echo after gadolinium administration.


Conclusion
Dual-echo Dixon can help to improve whole-heart CMRA image quality significantly. The additional whole-heart fat information delivered by this approach can support a number of new clinical studies addressing the diagnostic and the predictive value of intramyocardial and extramyocardial fatty deposits. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24616" xmlns="http://purl.org/rss/1.0/"><title>3D-mapping of phosphocreatine concentration in the human calf muscle at 7 T: comparison to 3 T</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24616</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">3D-mapping of phosphocreatine concentration in the human calf muscle at 7 T: comparison to 3 T</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Prodromos Parasoglou, Ding Xia, Gregory Chang, Ravinder R. Regatte</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-06T09:38:34.10637-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24616</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24616</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24616</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24616-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The development and implementation of a spectrally selective 3D-Turbo Spin Echo sequence for quantitative mapping of phosphocreatine (PCr) concentration in different muscles of the lower leg of healthy volunteers both at 3 T and 7 T.</p></div></div>
<div class="section" id="mrm24616-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Nine healthy volunteers were recruited, all of whom where scanned at 3 T and 7 T. Three dimensional PCr concentration maps were obtained after images were corrected for <em>B</em><sub>1</sub> inhomogeneities, <em>T</em><sub>1</sub> relaxation weighting, and partial volume of fatty tissue in the muscles. Two volunteers performed plantar flexions inside the magnet, and the oxidative capacity of their muscles was estimated.</p></div></div>
<div class="section" id="mrm24616-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Three dimensional PCr concentration maps were obtained, with full muscle coverage and nominal voxel size of 0.52 mL at both fields. At 7 T a 2.7-fold increase of signal-to-noise ratio was achieved compared to 3 T.</p></div></div>
<div class="section" id="mrm24616-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Imaging <sup>31</sup>P metabolites at 7 T allowed for significant increase in signal to noise ratio compared to imaging at 3 T, while quantification of the PCr concentration remained unaffected. The importance of such an increase in signal-to-noise ratio is 2-fold, first higher resolution images with reduced partial volume effects can be acquired, and second multiple measurements such as dynamic imaging of PCr post-exercise, <sup>31</sup>P magnetization transfer, or other <sup>1</sup>H measurements, can be acquired in a single imaging session. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
The development and implementation of a spectrally selective 3D-Turbo Spin Echo sequence for quantitative mapping of phosphocreatine (PCr) concentration in different muscles of the lower leg of healthy volunteers both at 3 T and 7 T.


Methods
Nine healthy volunteers were recruited, all of whom where scanned at 3 T and 7 T. Three dimensional PCr concentration maps were obtained after images were corrected for B1 inhomogeneities, T1 relaxation weighting, and partial volume of fatty tissue in the muscles. Two volunteers performed plantar flexions inside the magnet, and the oxidative capacity of their muscles was estimated.


Results
Three dimensional PCr concentration maps were obtained, with full muscle coverage and nominal voxel size of 0.52 mL at both fields. At 7 T a 2.7-fold increase of signal-to-noise ratio was achieved compared to 3 T.


Conclusion
Imaging 31P metabolites at 7 T allowed for significant increase in signal to noise ratio compared to imaging at 3 T, while quantification of the PCr concentration remained unaffected. The importance of such an increase in signal-to-noise ratio is 2-fold, first higher resolution images with reduced partial volume effects can be acquired, and second multiple measurements such as dynamic imaging of PCr post-exercise, 31P magnetization transfer, or other 1H measurements, can be acquired in a single imaging session. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24619" xmlns="http://purl.org/rss/1.0/"><title>Cationized ferritin as a magnetic resonance imaging probe to detect microstructural changes in a rat model of non-alcoholic steatohepatitis</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24619</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cationized ferritin as a magnetic resonance imaging probe to detect microstructural changes in a rat model of non-alcoholic steatohepatitis</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Scott C. Beeman, Lawrence J. Mandarino, Joseph F. Georges, Kevin M. Bennett</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-06T09:36:55.536486-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24619</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24619</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24619</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24619-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The goal of this work was to detect disease-related microstructural changes to the liver using magnetic resonance imaging. Chronic liver disease can cause microstructural changes in the liver that reduce plasma access to the perisinusoidal space—the site of exchange between the blood plasma and the hepatic parenchyma. The reduced plasma access to the perisinusoidal space inhibits hepatic function and contributes to the ∼30,000 chronic liver disease-related deaths per year.</p></div></div>
<div class="section" id="mrm24619-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>The extracellular matrix-specific cationized ferritin magnetic resonance imaging probe was injected intravenously into healthy rats and a rat model of the chronic liver disease non-alcoholic steatohepatitis. Rats were subsequently imaged with 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24619/asset/equation/mrm24619-math-0001.gif?v=1&amp;t=hh1lk4m6&amp;s=ada4a4b86ccbb9ff81e7daf4693bb3fdd2a8dc37" class="inlineGraphic"/>-weighted magnetic resonance imaging.</p></div></div>
<div class="section" id="mrm24619-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>This work demonstrates that the binding of cationized ferritin to the perisinusoidal extracellular matrix is reduced by 55% in a rat model of non-alcoholic steatohepatitis compared to healthy controls. This reduced binding is detectable in vivo with magnetic resonance imaging. Immunofluorescence and electron microscopy indicated that the reduced binding is due to inhibited macromolecular access to the perisinusoidal space caused by non-alcoholic steatohepatitis-related microstructural changes.</p></div></div>
<div class="section" id="mrm24619-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>The reduced accumulation of intravenously injected cationized ferritin may report on changes in macromolecular access to the liver parenchyma in chronic liver disease. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The goal of this work was to detect disease-related microstructural changes to the liver using magnetic resonance imaging. Chronic liver disease can cause microstructural changes in the liver that reduce plasma access to the perisinusoidal space—the site of exchange between the blood plasma and the hepatic parenchyma. The reduced plasma access to the perisinusoidal space inhibits hepatic function and contributes to the ∼30,000 chronic liver disease-related deaths per year.


Methods
The extracellular matrix-specific cationized ferritin magnetic resonance imaging probe was injected intravenously into healthy rats and a rat model of the chronic liver disease non-alcoholic steatohepatitis. Rats were subsequently imaged with 
T2*-weighted magnetic resonance imaging.


Results
This work demonstrates that the binding of cationized ferritin to the perisinusoidal extracellular matrix is reduced by 55% in a rat model of non-alcoholic steatohepatitis compared to healthy controls. This reduced binding is detectable in vivo with magnetic resonance imaging. Immunofluorescence and electron microscopy indicated that the reduced binding is due to inhibited macromolecular access to the perisinusoidal space caused by non-alcoholic steatohepatitis-related microstructural changes.


Conclusions
The reduced accumulation of intravenously injected cationized ferritin may report on changes in macromolecular access to the liver parenchyma in chronic liver disease. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24621" xmlns="http://purl.org/rss/1.0/"><title>Compressed sensing reconstruction improves sensitivity of variable density spiral fMRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24621</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Compressed sensing reconstruction improves sensitivity of variable density spiral fMRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">D. J. Holland, C. Liu, X. Song, E. L. Mazerolle, M. T. Stevens, A. J. Sederman, L. F. Gladden, R. C. N. D'Arcy, C. V. Bowen, S. D. Beyea</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-06T09:36:06.740621-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24621</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24621</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24621</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24621-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Functional MRI (fMRI) techniques that can provide excellent blood oxygen level dependent contrast, rapid whole brain imaging, and minimal spatial distortion are in demand. This study explored whether fMRI sensitivity can be improved through the use of compressed sensing (CS) reconstruction of variable density spiral fMRI.</p></div></div>
<div class="section" id="mrm24621-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Three different CS-reconstructed 1-shot variable density spirals were explored (corresponding to 28%, 35%, and 46% under-sampling), and compared with conventional 1-shot and 2-shot Archimedean spirals acquired using matched echo time and volume repetition time. fMRI maps were reconstructed with or without CS MRI and sensitivity was compared using identically matched voxels.</p></div></div>
<div class="section" id="mrm24621-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The results demonstrated that an l<sub>1</sub>-norm based CS reconstruction only led to an increase in functional contrast when applied to 28% under-sampled data. A whole brain <em>t</em>-contrast map revealed that 2-shot uniformly sampled spiral and 28% under-sampled spiral data reconstructed with CS yield equivalent sensitivity, even with matched echo time and volume repetition time</p></div></div>
<div class="section" id="mrm24621-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>VD spiral exhibits a useful operating range, in the region of 25–30% under-sampling, for which CS reconstruction can be used to increase the sensitivity of fMRI to brain activity. Using CS, VD acquisitions achieve the same sensitivity as 2-shot Archimedean acquisitions, but require only a single shot. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
Functional MRI (fMRI) techniques that can provide excellent blood oxygen level dependent contrast, rapid whole brain imaging, and minimal spatial distortion are in demand. This study explored whether fMRI sensitivity can be improved through the use of compressed sensing (CS) reconstruction of variable density spiral fMRI.


Methods
Three different CS-reconstructed 1-shot variable density spirals were explored (corresponding to 28%, 35%, and 46% under-sampling), and compared with conventional 1-shot and 2-shot Archimedean spirals acquired using matched echo time and volume repetition time. fMRI maps were reconstructed with or without CS MRI and sensitivity was compared using identically matched voxels.


Results
The results demonstrated that an l1-norm based CS reconstruction only led to an increase in functional contrast when applied to 28% under-sampled data. A whole brain t-contrast map revealed that 2-shot uniformly sampled spiral and 28% under-sampled spiral data reconstructed with CS yield equivalent sensitivity, even with matched echo time and volume repetition time


Conclusion
VD spiral exhibits a useful operating range, in the region of 25–30% under-sampling, for which CS reconstruction can be used to increase the sensitivity of fMRI to brain activity. Using CS, VD acquisitions achieve the same sensitivity as 2-shot Archimedean acquisitions, but require only a single shot. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24606" xmlns="http://purl.org/rss/1.0/"><title>Monitoring and compensating phase imperfections in cine balanced steady-state free precession</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24606</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Monitoring and compensating phase imperfections in cine balanced steady-state free precession</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Rudolf Fritz Fischer, Christoph Barmet, Markus Rudin, Peter Boesiger, Klaas Paul Pruessmann, Sebastian Kozerke</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-06T09:35:38.975196-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24606</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24606</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24606</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24606-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To analyze and correct for eddy current-induced phase imperfections in cardiac cine balanced steady-state free precession (bSSFP) imaging.</p></div></div>
<div class="section" id="mrm24606-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Eddy current-induced phase offsets were measured for different phase-encoding schemes using a higher order dynamic field camera. Based on these measurements, offset phases were corrected for in postprocessing and by run-time phase compensation applying radiofrequency phase increments and additional compensatory gradient areas. The findings were validated using numerical simulations, phantom experiments, and in vivo cardiac scans.</p></div></div>
<div class="section" id="mrm24606-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Depending on the phase-encoding scheme, significant eddy current-induced phase offsets were detected. Time-varying phase offsets were observed at subsequent excitations leading to steady-state distortions and hence to profile-dependent amplitude modulations in k-space. Taking into account measured k-space trajectories algebraic image reconstruction allowed compensating imperfect spatial encoding. Correction of amplitude modulations was successfully accomplished by run-time phase compensation.</p></div></div>
<div class="section" id="mrm24606-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Using magnetic field monitoring, artifacts in cine balanced steady-state free precession caused by uncompensated eddy current fields can be significantly reduced. <b>Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>

Purpose
To analyze and correct for eddy current-induced phase imperfections in cardiac cine balanced steady-state free precession (bSSFP) imaging.


Methods
Eddy current-induced phase offsets were measured for different phase-encoding schemes using a higher order dynamic field camera. Based on these measurements, offset phases were corrected for in postprocessing and by run-time phase compensation applying radiofrequency phase increments and additional compensatory gradient areas. The findings were validated using numerical simulations, phantom experiments, and in vivo cardiac scans.


Results
Depending on the phase-encoding scheme, significant eddy current-induced phase offsets were detected. Time-varying phase offsets were observed at subsequent excitations leading to steady-state distortions and hence to profile-dependent amplitude modulations in k-space. Taking into account measured k-space trajectories algebraic image reconstruction allowed compensating imperfect spatial encoding. Correction of amplitude modulations was successfully accomplished by run-time phase compensation.


Conclusion
Using magnetic field monitoring, artifacts in cine balanced steady-state free precession caused by uncompensated eddy current fields can be significantly reduced. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24620" xmlns="http://purl.org/rss/1.0/"><title>Correction for the T1 effect incorporating flip angle estimated by Kalman filter in cardiac-gated functional MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24620</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Correction for the T1 effect incorporating flip angle estimated by Kalman filter in cardiac-gated functional MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jaemin Shin, Sinyeob Ahn, Xiaoping Hu</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-06T09:19:51.160944-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24620</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24620</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24620</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>To develop an improved and generalized technique for correcting T1-related signal fluctuations (T1 effect) in cardiac-gated functional magnetie resonance imaging (fMRI) data with flip angle estimation.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods:</h4><div class="para"><p>Spatial maps of flip angle and T1 are jointly estimated from cardiac-gated time series using a Kalman filter. These maps are subsequently used for removing the T1 effect in the presence of B1 inhomogeneity. The new technique was compared with a prior technique that uses T1 only while assuming a homogeneous flip angle of 90°. The robustness of the new technique is demonstrated with simulated and experimental data.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>Simulation results revealed that the new method led to increased temporal signal-to-noise ratio across a large range of flip angles, T1s, and stimulus onset asynchrony means compared to the T1 only approach. With the experimental data, the new approach resulted in higher average gray matter temporal signal-to-noise ratio of seven subjects (84 vs. 48). The new approach also led to a higher statistical score of activation in the lateral geniculate nucleus (<em>P</em> &lt; 0.002).</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>The new technique is able to remove the T1 effect robustly and is a promising tool for improving the ability to map activation in fMRI, especially in subcortical regions. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
To develop an improved and generalized technique for correcting T1-related signal fluctuations (T1 effect) in cardiac-gated functional magnetie resonance imaging (fMRI) data with flip angle estimation.


Theory and Methods:
Spatial maps of flip angle and T1 are jointly estimated from cardiac-gated time series using a Kalman filter. These maps are subsequently used for removing the T1 effect in the presence of B1 inhomogeneity. The new technique was compared with a prior technique that uses T1 only while assuming a homogeneous flip angle of 90°. The robustness of the new technique is demonstrated with simulated and experimental data.


Results:
Simulation results revealed that the new method led to increased temporal signal-to-noise ratio across a large range of flip angles, T1s, and stimulus onset asynchrony means compared to the T1 only approach. With the experimental data, the new approach resulted in higher average gray matter temporal signal-to-noise ratio of seven subjects (84 vs. 48). The new approach also led to a higher statistical score of activation in the lateral geniculate nucleus (P &lt; 0.002).


Conclusion:
The new technique is able to remove the T1 effect robustly and is a promising tool for improving the ability to map activation in fMRI, especially in subcortical regions. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24609" xmlns="http://purl.org/rss/1.0/"><title>Determination of volume–time curves for the right ventricle and its outflow tract for functional analyses</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24609</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Determination of volume–time curves for the right ventricle and its outflow tract for functional analyses</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dominik D. Gabbert, Andreas Entenmann, Michael Jerosch-Herold, Felicitas Frettlöh, Christopher Hart, Inga Voges, Minh Pham, Ana Andrade, Eileen Pardun, P. Wegner, Traudel Hansen, Hans-Heiner Kramer, Carsten Rickers</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-04T09:30:33.306069-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24609</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24609</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24609</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24609-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The determination of right ventricular volumes and function is of increasing interest for the postoperative care of patients with congenital heart defects. The presentation of volumetry data in terms of volume-time curves allows a comprehensive functional assessment. By using manual contour tracing, the generation of volume–time curves is exceedingly time-consuming.</p></div></div>
<div class="section" id="mrm24609-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>This study describes a fast and precise method for determining volume–time curves for the right ventricle and for the right ventricular outflow tract. The method applies contour detection and includes a feature for identifying the right ventricular outflow tract volume. The segregation of the outflow tract is performed by four-dimensional curved smooth boundary surfaces defined by prespecified anatomical landmarks.</p></div></div>
<div class="section" id="mrm24609-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The comparison with manual contour tracing demonstrates that the method is accurate and improves the precision of the measurement. Compared to manual contour tracing the bias is &lt;0.1% ± 4.1% (right ventricle) and −2.6% ± 20.0% (right ventricular outflow tract). The standard deviations of inter- and intraobserver variabilities for determining the volume of the right ventricular outflow tract are reduced to less than half the values of manual contour tracing. The time consumption per patient is reduced from 341 ± 80 min (right ventricle) and 56 ± 11 min (right ventricular outflow tract) using manual contour tracing to 46 ± 9 min for a combined analysis of right ventricle and right ventricular outflow tract.</p></div></div>
<div class="section" id="mrm24609-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>The analysis of volume–time curves for the right ventricle and its outflow tract discloses new evaluation methods in clinical routine and science. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The determination of right ventricular volumes and function is of increasing interest for the postoperative care of patients with congenital heart defects. The presentation of volumetry data in terms of volume-time curves allows a comprehensive functional assessment. By using manual contour tracing, the generation of volume–time curves is exceedingly time-consuming.


Methods
This study describes a fast and precise method for determining volume–time curves for the right ventricle and for the right ventricular outflow tract. The method applies contour detection and includes a feature for identifying the right ventricular outflow tract volume. The segregation of the outflow tract is performed by four-dimensional curved smooth boundary surfaces defined by prespecified anatomical landmarks.


Results
The comparison with manual contour tracing demonstrates that the method is accurate and improves the precision of the measurement. Compared to manual contour tracing the bias is &lt;0.1% ± 4.1% (right ventricle) and −2.6% ± 20.0% (right ventricular outflow tract). The standard deviations of inter- and intraobserver variabilities for determining the volume of the right ventricular outflow tract are reduced to less than half the values of manual contour tracing. The time consumption per patient is reduced from 341 ± 80 min (right ventricle) and 56 ± 11 min (right ventricular outflow tract) using manual contour tracing to 46 ± 9 min for a combined analysis of right ventricle and right ventricular outflow tract.


Conclusion
The analysis of volume–time curves for the right ventricle and its outflow tract discloses new evaluation methods in clinical routine and science. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24598" xmlns="http://purl.org/rss/1.0/"><title>
B1+-mapping with the transient phase of unbalanced steady-state free precession</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24598</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">
B1+-mapping with the transient phase of unbalanced steady-state free precession</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Carl Ganter, Marcus Settles, Isabel Dregely, Francesco Santini, Klaus Scheffler, Oliver Bieri</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-04T09:30:17.636717-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24598</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24598</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24598</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24598-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>A novel 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24598/asset/equation/mrm24598-math-0003.gif?v=1&amp;t=hh1lk4n1&amp;s=911f11797d254c32038397ac73a361fcefcb1467" class="inlineGraphic"/>-mapping technique (B1-TRAP) is presented, which derives the actual flip angle from the frequency of signal oscillations, observed in the transient phase of unbalanced steady-state free precession sequences.</p></div></div>
<div class="section" id="mrm24598-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory</h4><div class="para"><p>For short repetition times (TR), the angular frequency of distinct oscillations in the transient phase of steady-state free precession sequences is proven to be approximately proportional to the actual flip angle: 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24598/asset/equation/mrm24598-math-0004.gif?v=1&amp;t=hh1lk4n2&amp;s=52379df10cffc01fd93072909f26eb1103428df0" class="inlineGraphic"/>. The result is not influenced by off-resonance and it can be shown that deviations are only of second order in the small parameter 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24598/asset/equation/mrm24598-math-0005.gif?v=1&amp;t=hh1lk4n2&amp;s=d37ea1e29e849a2052d736794be0ebb7329f2443" class="inlineGraphic"/>.</p></div></div>
<div class="section" id="mrm24598-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>B1-TRAP makes use of this effect through a frequency analysis of the transient phase of a train of steady-state free precession signals.</p></div></div>
<div class="section" id="mrm24598-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>In terms of reliability and time efficiency, a two-dimensional multislice implementation was found to be optimal. Unlike many steady-state 
<img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/mrm.24598/asset/equation/mrm24598-math-0006.gif?v=1&amp;t=hh1lk4n3&amp;s=46abfc9d7a2ea38fee2b9565b38b7b2b735d5fe1" class="inlineGraphic"/>-mapping methods, the accuracy of B1-TRAP was not impaired by imperfect slice profiles.</p></div></div>
<div class="section" id="mrm24598-sec-0005" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Simulations, phantom, and in vivo measurements showed that B1-TRAP offers a good compromise with respect to speed, robustness, and accuracy. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
A novel 
B1+-mapping technique (B1-TRAP) is presented, which derives the actual flip angle from the frequency of signal oscillations, observed in the transient phase of unbalanced steady-state free precession sequences.


Theory
For short repetition times (TR), the angular frequency of distinct oscillations in the transient phase of steady-state free precession sequences is proven to be approximately proportional to the actual flip angle: 
ω⋅TR≈α. The result is not influenced by off-resonance and it can be shown that deviations are only of second order in the small parameter 
TR/T2.


Methods
B1-TRAP makes use of this effect through a frequency analysis of the transient phase of a train of steady-state free precession signals.


Results
In terms of reliability and time efficiency, a two-dimensional multislice implementation was found to be optimal. Unlike many steady-state 
B1+-mapping methods, the accuracy of B1-TRAP was not impaired by imperfect slice profiles.


Conclusion
Simulations, phantom, and in vivo measurements showed that B1-TRAP offers a good compromise with respect to speed, robustness, and accuracy. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24629" xmlns="http://purl.org/rss/1.0/"><title>On the role of neuronal magnetic susceptibility and structure symmetry on gradient echo MR signal formation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24629</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">On the role of neuronal magnetic susceptibility and structure symmetry on gradient echo MR signal formation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Alexander L. Sukstanskii, Dmitriy A. Yablonskiy</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-04T09:28:25.43799-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24629</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24629</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24629</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24629-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Phase images obtained by gradient-recalled echo (GRE) MRI provide new contrast in the brain that is distinct from that obtained with conventional T1-weighted and T2-weighted images. The results are especially intriguing in white matter where both signal amplitude and phase display anisotropic properties. However, the biophysical origins of these phenomena are not well understood. The goal of this article is to provide a comprehensive theory of GRE signal formation based on a realistic model of neuronal structure.</p></div></div>
<div class="section" id="mrm24629-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>We use Maxwell equations to find the distribution of magnetic field induced by myelin sheath and axon. We account for both anisotropy of neuronal tissue “magnetic micro-architecture” and anisotropy of myelin sheath magnetic susceptibility.</p></div></div>
<div class="section" id="mrm24629-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Model describes GRE signal comprising of three compartments—axonal, myelin, and extracellular. Both axonal and myelin water signals have frequency shifts that are affected by the magnetic susceptibility anisotropy of long molecules forming lipid bilayer membranes. These parts of frequency shifts reach extrema for axon oriented perpendicular to the magnetic field and are zeros in a parallel case. Myelin water signal is substantially non-monoexponential.</p></div></div>
<div class="section" id="mrm24629-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>Both, anisotropy of neuronal tissue “magnetic micro-architecture” and anisotropy of myelin sheath magnetic susceptibility, are important for describing GRE signal phaseand magnitude. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Phase images obtained by gradient-recalled echo (GRE) MRI provide new contrast in the brain that is distinct from that obtained with conventional T1-weighted and T2-weighted images. The results are especially intriguing in white matter where both signal amplitude and phase display anisotropic properties. However, the biophysical origins of these phenomena are not well understood. The goal of this article is to provide a comprehensive theory of GRE signal formation based on a realistic model of neuronal structure.


Methods
We use Maxwell equations to find the distribution of magnetic field induced by myelin sheath and axon. We account for both anisotropy of neuronal tissue “magnetic micro-architecture” and anisotropy of myelin sheath magnetic susceptibility.


Results
Model describes GRE signal comprising of three compartments—axonal, myelin, and extracellular. Both axonal and myelin water signals have frequency shifts that are affected by the magnetic susceptibility anisotropy of long molecules forming lipid bilayer membranes. These parts of frequency shifts reach extrema for axon oriented perpendicular to the magnetic field and are zeros in a parallel case. Myelin water signal is substantially non-monoexponential.


Conclusions
Both, anisotropy of neuronal tissue “magnetic micro-architecture” and anisotropy of myelin sheath magnetic susceptibility, are important for describing GRE signal phaseand magnitude. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24604" xmlns="http://purl.org/rss/1.0/"><title>A variability study of regional alveolar oxygen tension measurement in humans using hyperpolarized 3He MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24604</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A variability study of regional alveolar oxygen tension measurement in humans using hyperpolarized 3He MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Hooman Hamedani, Stephen J. Kadlecek, Masaru Ishii, Kiarash Emami, Nicholas N. Kuzma, Yi Xin, Milton Rossman, Rahim R. Rizi</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-04T09:28:16.169905-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24604</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24604</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24604</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24604-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>A systematic study of the short-term and long-term variability of regional alveolar partial pressure of oxygen tension (<em>p</em><sub>A</sub>O<sub>2</sub>) measurements using <sup>3</sup>He magnetic resonance imaging was presented. Additionally, the repeatability of the average evaluated <em>p</em><sub>A</sub>O<sub>2</sub> was compared with that of the standard pulmonary function tests.</p></div></div>
<div class="section" id="mrm24604-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Pulmonary function test and <em>p</em><sub>A</sub>O<sub>2</sub> imaging were performed on 4 nonsmokers (1 M, 3 F, 56 ± 1.7 years) and 4 smokers (3 M, 1 F, 52 ± 7.5 years) during three visits over the course of 2 weeks. Two measurements were performed per visit. Variability of <em>p</em><sub>A</sub>O<sub>2</sub> was assessed using a mixed-effect model, with an intraclass correlation coefficient calculated for each group. The coefficient of variation of <em>p</em><sub>A</sub>O<sub>2</sub> over the 3-day period was also compared with the coefficient of variation of pulmonary function test results.</p></div></div>
<div class="section" id="mrm24604-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Short-term regional variability based on intraclass correlation coefficient was 0.71 for nonsmokers, and 0.63 for smokers, with long-term variability significantly lower at 0.59 and 0.47, respectively. While the coefficient of variation of the average <em>p</em><sub>A</sub>O<sub>2</sub> was similar to the repeatability of the diffusing capacity of CO, it was significantly higher than that of Forced Vital Capacity (<em>P</em> = 0.02).</p></div></div>
<div class="section" id="mrm24604-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Short-term and long-term <em>p</em><sub>A</sub>O<sub>2</sub> variability differences were used as an indication of true physiological changes in order to measure technical reproducibility. Smokers show higher physiologic variability and less technical reproducibility. The suggested <em>p</em><sub>A</sub>O<sub>2</sub>-imaging technique showed a reasonable regional repeatability in nonsmokers as well as the ability to detect differences between the two groups with similar reproducibility and superior discriminatory ability when compared with pulmonary function tests. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
A systematic study of the short-term and long-term variability of regional alveolar partial pressure of oxygen tension (pAO2) measurements using 3He magnetic resonance imaging was presented. Additionally, the repeatability of the average evaluated pAO2 was compared with that of the standard pulmonary function tests.


Methods
Pulmonary function test and pAO2 imaging were performed on 4 nonsmokers (1 M, 3 F, 56 ± 1.7 years) and 4 smokers (3 M, 1 F, 52 ± 7.5 years) during three visits over the course of 2 weeks. Two measurements were performed per visit. Variability of pAO2 was assessed using a mixed-effect model, with an intraclass correlation coefficient calculated for each group. The coefficient of variation of pAO2 over the 3-day period was also compared with the coefficient of variation of pulmonary function test results.


Results
Short-term regional variability based on intraclass correlation coefficient was 0.71 for nonsmokers, and 0.63 for smokers, with long-term variability significantly lower at 0.59 and 0.47, respectively. While the coefficient of variation of the average pAO2 was similar to the repeatability of the diffusing capacity of CO, it was significantly higher than that of Forced Vital Capacity (P = 0.02).


Conclusion
Short-term and long-term pAO2 variability differences were used as an indication of true physiological changes in order to measure technical reproducibility. Smokers show higher physiologic variability and less technical reproducibility. The suggested pAO2-imaging technique showed a reasonable regional repeatability in nonsmokers as well as the ability to detect differences between the two groups with similar reproducibility and superior discriminatory ability when compared with pulmonary function tests. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24614" xmlns="http://purl.org/rss/1.0/"><title>Dynamic imaging of the fetal heart using metric optimized gating</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24614</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Dynamic imaging of the fetal heart using metric optimized gating</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Christopher W. Roy, Mike Seed, Joshua F. P. Amerom, Bahiyah Nafisi, Lars Grosse-Wortmann, Shi-Joon Yoo, Christopher K. Macgowan</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-02-04T09:28:00.587835-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24614</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24614</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24614</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24614-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>Advances in fetal cardiovascular magnetic resonance imaging have been limited by the absence of a reliable cardiac gating signal. The purpose of this work was to develop and validate metric-optimized gating (MOG) for cine imaging of the fetal heart.</p></div></div>
<div class="section" id="mrm24614-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods</h4><div class="para"><p>Cine MR and electrocardiogram data were acquired in healthy adult volunteers for validation of the MOG method. Comparison of MOG and electrocardiogram reconstructions was performed based on the image quality for each method, and the difference between MOG and electrocardiogram trigger times. Fetal images were also acquired, their quality evaluated by experienced radiologists, and the theoretical error in the MOG trigger times were calculated.</p></div></div>
<div class="section" id="mrm24614-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Excellent agreement between electrocardiogram and MOG reconstructions was observed. The experimental errors in adult MOG trigger times for all five volunteers were ±(7,25, 17, 8, and 13) ms. Fetal images captured normal and diseased cardiac dynamics.</p></div></div>
<div class="section" id="mrm24614-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>MOG for cine imaging of the fetal myocardium was developed and validated in adults. Using MOG, the first gated MR images of the human fetal myocardium were obtained. Small moving structures were visualized during radial contraction, thus capturing normal fetal cardiac wall motion and permitting assessment of cardiac function. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
Advances in fetal cardiovascular magnetic resonance imaging have been limited by the absence of a reliable cardiac gating signal. The purpose of this work was to develop and validate metric-optimized gating (MOG) for cine imaging of the fetal heart.


Theory and Methods
Cine MR and electrocardiogram data were acquired in healthy adult volunteers for validation of the MOG method. Comparison of MOG and electrocardiogram reconstructions was performed based on the image quality for each method, and the difference between MOG and electrocardiogram trigger times. Fetal images were also acquired, their quality evaluated by experienced radiologists, and the theoretical error in the MOG trigger times were calculated.


Results
Excellent agreement between electrocardiogram and MOG reconstructions was observed. The experimental errors in adult MOG trigger times for all five volunteers were ±(7,25, 17, 8, and 13) ms. Fetal images captured normal and diseased cardiac dynamics.


Conclusion
MOG for cine imaging of the fetal myocardium was developed and validated in adults. Using MOG, the first gated MR images of the human fetal myocardium were obtained. Small moving structures were visualized during radial contraction, thus capturing normal fetal cardiac wall motion and permitting assessment of cardiac function. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24605" xmlns="http://purl.org/rss/1.0/"><title>Accelerated MRI by SPEED with generalized sampling schemes</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24605</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Accelerated MRI by SPEED with generalized sampling schemes</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Zhaoyang Jin, Qing-San Xiang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-30T17:05:31.053936-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24605</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24605</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24605</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24605-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To enhance the fast imaging technique of skipped phase encoding (PE) and edge deghosting (SPEED) for more general sampling options, and thus more flexibility in implementations and applications.</p></div></div>
<div class="section" id="mrm24605-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>SPEED uses skipped PE steps to accelerate MRI scan. Previously, the PE skip size was chosen from prime numbers only. This restriction has been relaxed in this study to allow choice of any integers rather than merely prime numbers. Various sampling patterns were studied under all possible combinations of PE skip size and PE shifts. A criterion based on the rank values of ghost phasor matrices was introduced to evaluate SPEED reconstruction.</p></div></div>
<div class="section" id="mrm24605-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The reconstruction quality was found to correlate with the rank value of the ghost phasor matrix and the skipped PE size <em>N</em>. A low-rank value indicates a singular matrix that causes failure of the SPEED reconstruction. Composite numbers combined with appropriately chosen PE shifts yielded satisfactory reconstruction results.</p></div></div>
<div class="section" id="mrm24605-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>With properly chosen PE shifts, it was found that any integers, including both prime numbers and composite numbers, could be used as PE skip size for SPEED. This finding allows much more flexible data acquisition options that may lead to more freedom in practical implementations and applications. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To enhance the fast imaging technique of skipped phase encoding (PE) and edge deghosting (SPEED) for more general sampling options, and thus more flexibility in implementations and applications.


Methods
SPEED uses skipped PE steps to accelerate MRI scan. Previously, the PE skip size was chosen from prime numbers only. This restriction has been relaxed in this study to allow choice of any integers rather than merely prime numbers. Various sampling patterns were studied under all possible combinations of PE skip size and PE shifts. A criterion based on the rank values of ghost phasor matrices was introduced to evaluate SPEED reconstruction.


Results
The reconstruction quality was found to correlate with the rank value of the ghost phasor matrix and the skipped PE size N. A low-rank value indicates a singular matrix that causes failure of the SPEED reconstruction. Composite numbers combined with appropriately chosen PE shifts yielded satisfactory reconstruction results.


Conclusion
With properly chosen PE shifts, it was found that any integers, including both prime numbers and composite numbers, could be used as PE skip size for SPEED. This finding allows much more flexible data acquisition options that may lead to more freedom in practical implementations and applications. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24602" xmlns="http://purl.org/rss/1.0/"><title>Reliability of two clinically relevant fiber pathways reconstructed with constrained spherical deconvolution</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24602</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Reliability of two clinically relevant fiber pathways reconstructed with constrained spherical deconvolution</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Gert Kristo, Alexander Leemans, Mathijs Raemaekers, Geert-Jan Rutten, Beatrice Gelder, Nick F. Ramsey</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-28T17:30:45.970086-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24602</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24602</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24602</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>The single diffusion tensor model is inadequate for the reconstruction of fiber pathways in brain regions with multiple fiber orientations. To overcome this limitation, constrained spherical deconvolution has been proposed. A high reliability of constrained spherical deconvolution is, however, a pre-requisite for its use in clinical applications. Reliability of reconstructed fiber pathways can be assessed in terms of architectural (addressing their spatial configuration) and microstructural (addressing diffusion-derived measures along the fibers) reproducibility. We assess the reliability for two clinically relevant fiber pathways: the corticospinal tract and arcuate fasciculus. The fiber pathways were reconstructed using constrained spherical deconvolution in 11 healthy subjects who were scanned on three occasions. Coefficients of variations of diffusion-derived measures were used to assess the microstructural reproducibility. Image correlation and fiber overlap were used to assess the architectural reproducibility. The mean correlation between sessions was 72% for both the corticospinal tract and arcuate fasciculus. The mean overlap between sessions was 63% for the corticospinal tract and 58% for the arcuate fasciculus. Coefficients of variations of diffusion-derived measures showed very low variation (all measures &lt;3.1%). These results are comparable with reliability results based on the diffusion tensor model, which is commonly used in clinical settings. The reliability results found here are, therefore, promising to further investigate the use of constrained spherical deconvolution in clinical practice. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div>
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The single diffusion tensor model is inadequate for the reconstruction of fiber pathways in brain regions with multiple fiber orientations. To overcome this limitation, constrained spherical deconvolution has been proposed. A high reliability of constrained spherical deconvolution is, however, a pre-requisite for its use in clinical applications. Reliability of reconstructed fiber pathways can be assessed in terms of architectural (addressing their spatial configuration) and microstructural (addressing diffusion-derived measures along the fibers) reproducibility. We assess the reliability for two clinically relevant fiber pathways: the corticospinal tract and arcuate fasciculus. The fiber pathways were reconstructed using constrained spherical deconvolution in 11 healthy subjects who were scanned on three occasions. Coefficients of variations of diffusion-derived measures were used to assess the microstructural reproducibility. Image correlation and fiber overlap were used to assess the architectural reproducibility. The mean correlation between sessions was 72% for both the corticospinal tract and arcuate fasciculus. The mean overlap between sessions was 63% for the corticospinal tract and 58% for the arcuate fasciculus. Coefficients of variations of diffusion-derived measures showed very low variation (all measures &lt;3.1%). These results are comparable with reliability results based on the diffusion tensor model, which is commonly used in clinical settings. The reliability results found here are, therefore, promising to further investigate the use of constrained spherical deconvolution in clinical practice. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24607" xmlns="http://purl.org/rss/1.0/"><title>Improved MRI R2* relaxometry of iron-loaded liver with noise correction</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24607</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Improved MRI R2* relaxometry of iron-loaded liver with noise correction</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Yanqiu Feng, Taigang He, Peter D. Gatehouse, Xinzhong Li, Mohammed Harith Alam, Dudley J. Pennell, Wufan Chen, David N. Firmin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-28T17:30:31.707627-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24607</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24607</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24607</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="para" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><p>Accurate and reproducible MRI <em>R</em><sub>2</sub>* relaxometry for tissue iron quantification is important in managing transfusion-dependent patients. MRI data are often acquired using array coils and reconstructed by the root-sum-square algorithm, and as such, measured signals follow the noncentral chi distribution. In this study, two noise-corrected models were proposed for the liver <em>R</em><sub>2</sub>* quantification: fitting the signal to the first moment and fitting the squared signal to the second moment in the presence of the noncentral chi noise. These two models were compared with the widely implemented offset and truncation models on both simulation and in vivo data. The results demonstrated that the “slow decay component” of the liver <em>R</em><sub>2</sub>* was mainly caused by the noise. The offset model considerably overestimated <em>R</em><sub>2</sub>* values by incorrectly adding a constant to account for the slow decay component. The truncation model generally produced accurate <em>R</em><sub>2</sub>* measurements by only fitting the initial data well above the noise level to remove the major source of errors, but underestimated very high <em>R</em><sub>2</sub>* values due to the sequence limit of obtaining very short echo time images. Both the first and second-moment noise-corrected models constantly produced accurate and precise <em>R</em><sub>2</sub>* measurements by correctly addressing the noise problem. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div>
]]></content:encoded><description>
Accurate and reproducible MRI R2* relaxometry for tissue iron quantification is important in managing transfusion-dependent patients. MRI data are often acquired using array coils and reconstructed by the root-sum-square algorithm, and as such, measured signals follow the noncentral chi distribution. In this study, two noise-corrected models were proposed for the liver R2* quantification: fitting the signal to the first moment and fitting the squared signal to the second moment in the presence of the noncentral chi noise. These two models were compared with the widely implemented offset and truncation models on both simulation and in vivo data. The results demonstrated that the “slow decay component” of the liver R2* was mainly caused by the noise. The offset model considerably overestimated R2* values by incorrectly adding a constant to account for the slow decay component. The truncation model generally produced accurate R2* measurements by only fitting the initial data well above the noise level to remove the major source of errors, but underestimated very high R2* values due to the sequence limit of obtaining very short echo time images. Both the first and second-moment noise-corrected models constantly produced accurate and precise R2* measurements by correctly addressing the noise problem. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24595" xmlns="http://purl.org/rss/1.0/"><title>Lung morphometry using hyperpolarized 129Xe apparent diffusion coefficient anisotropy in chronic obstructive pulmonary disease</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24595</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Lung morphometry using hyperpolarized 129Xe apparent diffusion coefficient anisotropy in chronic obstructive pulmonary disease</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Alexei Ouriadov, Adam Farag, Miranda Kirby, David G. McCormack, Grace Parraga, Giles E. Santyr</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-28T17:30:27.863824-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24595</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24595</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24595</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24595-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>The goal of this work was to investigate lung morphological changes associated with chronic obstructive pulmonary disease (COPD) using hyperpolarized <sup>129</sup>Xe diffusion-weighted MRI.</p></div></div>
<div class="section" id="mrm24595-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Hyperpolarized <sup>129</sup>Xe MRI was performed at three different nonzero diffusion sensitizations (<em>b</em>-value = 12, 20, and 30 s/cm<sup>2</sup>) in the lungs of four subjects with COPD and four healthy volunteers. The image signal intensities were fit as a function of <em>b</em>-value to obtain anisotropic diffusion coefficient maps for all subjects. The image signal intensities were also fit to a morphological model allowing extraction of length scales associated with the terminal airways: external radius (<em>R</em>), internal radius (<em>r</em>), mean airspace chord length (<em>L</em><sub>m</sub>), and depth of alveolar sleeve (<em>h</em>).</p></div></div>
<div class="section" id="mrm24595-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Longitudinal (<em>D</em><sub>L</sub>) and transverse (<em>D</em><sub>T</sub>) anisotropic diffusion coefficients were both significantly increased (both <em>P</em>= 0.004) in the COPD subjects (0.102 ± 0.02 cm<sup>2</sup>/s and 0.072 ± 0.02 cm<sup>2</sup>/s, respectively) compared with the healthy subjects (0.083 ± 0.011 cm<sup>2</sup>/s and 0.046 ± 0.017 cm<sup>2</sup>/s, respectively). Significant morphological differences were observed between the COPD subjects and healthy volunteers, specifically decreases in <em>h</em> (68 ± 36 µm vs. 95 ± 710 µm, respectively, <em>P</em> = 0.019) and increases in <em>L</em><sub>m</sub> (352 ± 57 µm vs. 253 ± 37 µm, respectively, <em>P</em> = 0.002) consistent with values obtained previously using hyperpolarized <sup>3</sup>He MRI in similar subjects.</p></div></div>
<div class="section" id="mrm24595-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>Diffusion-weighted hyperpolarized <sup>129</sup>Xe MRI is a promising technique for mapping changes in human lung morphology and may be useful for early detection of emphysema associated with COPD. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
The goal of this work was to investigate lung morphological changes associated with chronic obstructive pulmonary disease (COPD) using hyperpolarized 129Xe diffusion-weighted MRI.


Methods
Hyperpolarized 129Xe MRI was performed at three different nonzero diffusion sensitizations (b-value = 12, 20, and 30 s/cm2) in the lungs of four subjects with COPD and four healthy volunteers. The image signal intensities were fit as a function of b-value to obtain anisotropic diffusion coefficient maps for all subjects. The image signal intensities were also fit to a morphological model allowing extraction of length scales associated with the terminal airways: external radius (R), internal radius (r), mean airspace chord length (Lm), and depth of alveolar sleeve (h).


Results
Longitudinal (DL) and transverse (DT) anisotropic diffusion coefficients were both significantly increased (both P= 0.004) in the COPD subjects (0.102 ± 0.02 cm2/s and 0.072 ± 0.02 cm2/s, respectively) compared with the healthy subjects (0.083 ± 0.011 cm2/s and 0.046 ± 0.017 cm2/s, respectively). Significant morphological differences were observed between the COPD subjects and healthy volunteers, specifically decreases in h (68 ± 36 µm vs. 95 ± 710 µm, respectively, P = 0.019) and increases in Lm (352 ± 57 µm vs. 253 ± 37 µm, respectively, P = 0.002) consistent with values obtained previously using hyperpolarized 3He MRI in similar subjects.


Conclusions
Diffusion-weighted hyperpolarized 129Xe MRI is a promising technique for mapping changes in human lung morphology and may be useful for early detection of emphysema associated with COPD. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24594" xmlns="http://purl.org/rss/1.0/"><title>Diffusion-weighted 3D multislab echo planar imaging for high signal-to-noise ratio efficiency and isotropic image resolution</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24594</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Diffusion-weighted 3D multislab echo planar imaging for high signal-to-noise ratio efficiency and isotropic image resolution</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mathias Engström, Stefan Skare</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-28T17:30:20.914865-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24594</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24594</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24594</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24594-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>To acquire isotropic high-resolution, signal-to-noise ratio (SNR) efficient, 3D encoded diffusion-weighted MRI data.</p></div></div>
<div class="section" id="mrm24594-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Multiple Fourier encoded slabs were combined into one full volume, using a generalized autocalibrating partially parallel acquisitions (GRAPPA) accelerated diffusion-weighted 3D multislab echo planar imaging (EPI) sequence with 2D phase navigation and in-plane motion correction.</p></div></div>
<div class="section" id="mrm24594-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>Reconstructed data with 1.5-mm<sup>3</sup> nominal resolution is presented and shown under the influence of motion and with variable slab thicknesses. The SNR efficiency between diffusion-weighted 3D multislab EPI and DW 2D ss-EPI is compared. Finally, a 1.3-mm<sup>3</sup> full brain scan with 45 diffusion directions is presented.</p></div></div>
<div class="section" id="mrm24594-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusions</h4><div class="para"><p>Diffusion-weighted 3D multislab EPI has been presented as an alternative sequence for high-resolution and high-SNR full brain coverage diffusion studies. Compared with the gold standard 2D diffusion-weighted single-shot Echo Planar Imaging, the SNR efficiency is significantly higher. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
To acquire isotropic high-resolution, signal-to-noise ratio (SNR) efficient, 3D encoded diffusion-weighted MRI data.


Methods
Multiple Fourier encoded slabs were combined into one full volume, using a generalized autocalibrating partially parallel acquisitions (GRAPPA) accelerated diffusion-weighted 3D multislab echo planar imaging (EPI) sequence with 2D phase navigation and in-plane motion correction.


Results
Reconstructed data with 1.5-mm3 nominal resolution is presented and shown under the influence of motion and with variable slab thicknesses. The SNR efficiency between diffusion-weighted 3D multislab EPI and DW 2D ss-EPI is compared. Finally, a 1.3-mm3 full brain scan with 45 diffusion directions is presented.


Conclusions
Diffusion-weighted 3D multislab EPI has been presented as an alternative sequence for high-resolution and high-SNR full brain coverage diffusion studies. Compared with the gold standard 2D diffusion-weighted single-shot Echo Planar Imaging, the SNR efficiency is significantly higher. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24593" xmlns="http://purl.org/rss/1.0/"><title>Multipeak fat-corrected complex R2* relaxometry: Theory, optimization, and clinical validation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24593</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Multipeak fat-corrected complex R2* relaxometry: Theory, optimization, and clinical validation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Diego Hernando, J. Harald Kramer, Scott B. Reeder</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-28T12:55:54.880671-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24593</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24593</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24593</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>To develop R2* mapping techniques corrected for confounding factors and optimized for noise performance.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods:</h4><div class="para"><p>Conventional R2* mapping is affected by two key confounding factors: noise-related bias and the presence of fat in tissue. Noise floor effects introduce bias in magnitude-based reconstructions, particularly at high R2* values. The presence of fat, if uncorrected, introduces severe protocol-dependent bias. In this work, the bias/noise properties of different R2* mapping reconstructions (magnitude- and complex-fitting, fat-uncorrected, and fat-corrected) are characterized using Cramer-Rao Bound analysis, simulations, and in vivo data. A framework for optimizing the choice of echo times is provided. Finally, the robustness of liver R2* mapping in the presence of fat is evaluated in 28 subjects.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>Fat-corrected R2* mapping removes fat-related bias without noise penalty over a wide range of R2* values. Complex nonlinear least-squares fitted and fat-corrected R2* reconstructions that account for the spectral complexity of fat provide robust R2* estimates with low bias and optimized noise performance over a wide range of echo times combinations and R2* values.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>The use of complex fitting and fat-correction improves the robustness, noise performance, and accuracy of R2* measurements, and are necessary to establish R2* as quantitative imaging biomarker in the liver. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
To develop R2* mapping techniques corrected for confounding factors and optimized for noise performance.


Theory and Methods:
Conventional R2* mapping is affected by two key confounding factors: noise-related bias and the presence of fat in tissue. Noise floor effects introduce bias in magnitude-based reconstructions, particularly at high R2* values. The presence of fat, if uncorrected, introduces severe protocol-dependent bias. In this work, the bias/noise properties of different R2* mapping reconstructions (magnitude- and complex-fitting, fat-uncorrected, and fat-corrected) are characterized using Cramer-Rao Bound analysis, simulations, and in vivo data. A framework for optimizing the choice of echo times is provided. Finally, the robustness of liver R2* mapping in the presence of fat is evaluated in 28 subjects.


Results:
Fat-corrected R2* mapping removes fat-related bias without noise penalty over a wide range of R2* values. Complex nonlinear least-squares fitted and fat-corrected R2* reconstructions that account for the spectral complexity of fat provide robust R2* estimates with low bias and optimized noise performance over a wide range of echo times combinations and R2* values.


Conclusion:
The use of complex fitting and fat-correction improves the robustness, noise performance, and accuracy of R2* measurements, and are necessary to establish R2* as quantitative imaging biomarker in the liver. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24596" xmlns="http://purl.org/rss/1.0/"><title>Quiescent-inflow single-shot magnetic resonance angiography using a highly undersampled radial k-space trajectory</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24596</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Quiescent-inflow single-shot magnetic resonance angiography using a highly undersampled radial k-space trajectory</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">R. R. Edelman, S. Giri, E. Dunkle, M. Galizia, P. Amin, I. Koktzoglou</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-24T09:56:40.952226-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24596</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24596</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24596</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<div class="section" id="mrm24596-sec-0001" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose</h4><div class="para"><p>We hypothesized that high undersampling factors could be used in conjunction with radial quiescent-inflow single-shot magnetic resonance angiography (MRA) to accelerate the data acquisition and enable multislice acquisitions.</p></div></div>
<div class="section" id="mrm24596-sec-0002" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods</h4><div class="para"><p>Seven subjects were imaged on a 1.5 T MRI system. For multislice quiescent-inflow single-shot MRA, the venous saturation radiofrequency pulse, in-plane saturation radiofrequency pulse, and quiescent interval were applied only once before the first slice.</p></div></div>
<div class="section" id="mrm24596-sec-0003" xmlns="http://www.w3.org/1999/xhtml"><h4>Results</h4><div class="para"><p>The mean (standard deviation) measurements for the intra-arterial signal-to-noise ratio were as follows: Cartesian 1 slice—29.3 (5.5); radial 1 slice, 92 views—22.3 (3.6); radial 1 slice, 46 views—18.5 (2.0); radial 2 slices, 46 views—18.3 (3.2); and radial 3 slices, 32 views—21.7 (3.9), normalized for pixel size to 15.8. Horizontal striping was present with multislice radial quiescent-inflow single-shot MRA (especially with the three-slice acquisition) due to variable <em>T</em><sub>1</sub> relaxation between the concurrently acquired slices, but the image quality remained diagnostic. Vascular pathology in patients with peripheral arterial disease was well shown by all techniques.</p></div></div>
<div class="section" id="mrm24596-sec-0004" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion</h4><div class="para"><p>Very high undersampling factors in excess of 18 have been demonstrated for nonenhanced MRA using a radial quiescent-inflow single-shot technique, enabling the acquisition of two to three slices per cardiac cycle. Scan time for a complete peripheral MRA could be shortened to 2 min or less. Magn Reson Med, 2013. © 2012 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>

Purpose
We hypothesized that high undersampling factors could be used in conjunction with radial quiescent-inflow single-shot magnetic resonance angiography (MRA) to accelerate the data acquisition and enable multislice acquisitions.


Methods
Seven subjects were imaged on a 1.5 T MRI system. For multislice quiescent-inflow single-shot MRA, the venous saturation radiofrequency pulse, in-plane saturation radiofrequency pulse, and quiescent interval were applied only once before the first slice.


Results
The mean (standard deviation) measurements for the intra-arterial signal-to-noise ratio were as follows: Cartesian 1 slice—29.3 (5.5); radial 1 slice, 92 views—22.3 (3.6); radial 1 slice, 46 views—18.5 (2.0); radial 2 slices, 46 views—18.3 (3.2); and radial 3 slices, 32 views—21.7 (3.9), normalized for pixel size to 15.8. Horizontal striping was present with multislice radial quiescent-inflow single-shot MRA (especially with the three-slice acquisition) due to variable T1 relaxation between the concurrently acquired slices, but the image quality remained diagnostic. Vascular pathology in patients with peripheral arterial disease was well shown by all techniques.


Conclusion
Very high undersampling factors in excess of 18 have been demonstrated for nonenhanced MRA using a radial quiescent-inflow single-shot technique, enabling the acquisition of two to three slices per cardiac cycle. Scan time for a complete peripheral MRA could be shortened to 2 min or less. Magn Reson Med, 2013. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24568" xmlns="http://purl.org/rss/1.0/"><title>Transverse relaxometry with reduced echo train lengths via stimulated echo compensation</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24568</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Transverse relaxometry with reduced echo train lengths via stimulated echo compensation</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Md. Nasir Uddin, R. Marc Lebel, Alan H. Wilman</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-16T11:17:16.239658-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24568</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24568</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24568</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Transverse relaxation (<em>T</em><sub>2</sub>) mapping has many applications, including imaging of iron accumulation in grey matter. Using the typical multiecho spin-echo sequence with long echo trains, stimulated echo compensation can enable <em>T</em><sub>2</sub> fitting under conditions of variable radio frequency homogeneity arising from slice profile and in-plane radio frequency variation. Substantial reduction in the number of refocusing pulses could enable use at high magnetic fields where specific absorption rate is a major limitation, and enable multislice use with reduced incidental magnetization transfer at all field strengths. We examine the effect of reduced echo train lengths and multislice imaging on <em>T</em><sub>2</sub> fitting using stimulated echo compensation applied to iron-rich subcortical grey matter in human brain at 4.7 T. Our findings indicate that reducing from 20 echoes to as few as four echoes can maintain consistent <em>T</em><sub>2</sub> values when using stimulated echo compensation in grey and white matter, but not for cerebrospinal fluid. All territories produce marginal results when using standard exponential fitting. Savings from reduced echoes can be used to substantially increase slice coverage. In multislice mode, the resulting incidental magnetization transfer decreased brain signal but had minimal effect on measured <em>T</em><sub>2</sub> values. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div>
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Transverse relaxation (T2) mapping has many applications, including imaging of iron accumulation in grey matter. Using the typical multiecho spin-echo sequence with long echo trains, stimulated echo compensation can enable T2 fitting under conditions of variable radio frequency homogeneity arising from slice profile and in-plane radio frequency variation. Substantial reduction in the number of refocusing pulses could enable use at high magnetic fields where specific absorption rate is a major limitation, and enable multislice use with reduced incidental magnetization transfer at all field strengths. We examine the effect of reduced echo train lengths and multislice imaging on T2 fitting using stimulated echo compensation applied to iron-rich subcortical grey matter in human brain at 4.7 T. Our findings indicate that reducing from 20 echoes to as few as four echoes can maintain consistent T2 values when using stimulated echo compensation in grey and white matter, but not for cerebrospinal fluid. All territories produce marginal results when using standard exponential fitting. Savings from reduced echoes can be used to substantially increase slice coverage. In multislice mode, the resulting incidental magnetization transfer decreased brain signal but had minimal effect on measured T2 values. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24589" xmlns="http://purl.org/rss/1.0/"><title>Prospective and retrospective high order eddy current mitigation for diffusion weighted echo planar imaging</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24589</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Prospective and retrospective high order eddy current mitigation for diffusion weighted echo planar imaging</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dan Xu, Joseph K. Maier, Kevin F. King, Bruce D. Collick, Gaohong Wu, Robert D. Peters, R. Scott Hinks</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-16T11:17:03.838532-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24589</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24589</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24589</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>The proposed method is aimed at reducing eddy current (EC) induced distortion in diffusion weighted echo planar imaging, without the need to perform further image coregistration between diffusion weighted and T2 images. These ECs typically have significant high order spatial components that cannot be compensated by preemphasis.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods:</h4><div class="para"><p>High order ECs are first calibrated at the system level in a protocol independent fashion. The resulting amplitudes and time constants of high order ECs can then be used to calculate imaging protocol specific corrections. A combined prospective and retrospective approach is proposed to apply correction during data acquisition and image reconstruction.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>Various phantom, brain, body, and whole body diffusion weighted images with and without the proposed method are acquired. Significantly reduced image distortion and misregistration are consistently seen in images with the proposed method compared with images without.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>The proposed method is a powerful (e.g., effective at 48 cm field of view and 30 cm slice coverage) and flexible (e.g., compatible with other image enhancements and arbitrary scan plane) technique to correct high order ECs induced distortion and misregistration for various diffusion weighted echo planar imaging applications, without the need for further image post processing, protocol dependent prescan, or sacrifice in signal-to-noise ratio. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
The proposed method is aimed at reducing eddy current (EC) induced distortion in diffusion weighted echo planar imaging, without the need to perform further image coregistration between diffusion weighted and T2 images. These ECs typically have significant high order spatial components that cannot be compensated by preemphasis.


Theory and Methods:
High order ECs are first calibrated at the system level in a protocol independent fashion. The resulting amplitudes and time constants of high order ECs can then be used to calculate imaging protocol specific corrections. A combined prospective and retrospective approach is proposed to apply correction during data acquisition and image reconstruction.


Results:
Various phantom, brain, body, and whole body diffusion weighted images with and without the proposed method are acquired. Significantly reduced image distortion and misregistration are consistently seen in images with the proposed method compared with images without.


Conclusion:
The proposed method is a powerful (e.g., effective at 48 cm field of view and 30 cm slice coverage) and flexible (e.g., compatible with other image enhancements and arbitrary scan plane) technique to correct high order ECs induced distortion and misregistration for various diffusion weighted echo planar imaging applications, without the need for further image post processing, protocol dependent prescan, or sacrifice in signal-to-noise ratio. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24567" xmlns="http://purl.org/rss/1.0/"><title>Optimal sampling schedule for chemical exchange saturation transfer</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24567</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Optimal sampling schedule for chemical exchange saturation transfer</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Y. K. Tee, A. A. Khrapitchev, N. R. Sibson, S. J. Payne, M. A. Chappell</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-11T10:04:08.287224-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24567</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24567</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24567</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>The sampling schedule for chemical exchange saturation transfer imaging is normally uniformly distributed across the saturation frequency offsets. When this kind of evenly distributed sampling schedule is used to quantify the chemical exchange saturation transfer effect using model-based analysis, some of the collected data are minimally informative to the parameters of interest. For example, changes in labile proton exchange rate and concentration mainly affect the magnetization near the resonance frequency of the labile pool. In this study, an optimal sampling schedule was designed for a more accurate quantification of amine proton exchange rate and concentration, and water center frequency shift based on an algorithm previously applied to magnetization transfer and arterial spin labeling. The resulting optimal sampling schedule samples repeatedly around the resonance frequency of the amine pool and also near to the water resonance to maximize the information present within the data for quantitative model-based analysis. Simulation and experimental results on tissue-like phantoms showed that greater accuracy and precision (&gt;30% and &gt;46%, respectively, for some cases) were achieved in the parameters of interest when using optimal sampling schedule compared with evenly distributed sampling schedule. Hence, the proposed optimal sampling schedule could replace evenly distributed sampling schedule in chemical exchange saturation transfer imaging to improve the quantification of the chemical exchange saturation transfer effect and parameter estimation. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div>
]]></content:encoded><description>

The sampling schedule for chemical exchange saturation transfer imaging is normally uniformly distributed across the saturation frequency offsets. When this kind of evenly distributed sampling schedule is used to quantify the chemical exchange saturation transfer effect using model-based analysis, some of the collected data are minimally informative to the parameters of interest. For example, changes in labile proton exchange rate and concentration mainly affect the magnetization near the resonance frequency of the labile pool. In this study, an optimal sampling schedule was designed for a more accurate quantification of amine proton exchange rate and concentration, and water center frequency shift based on an algorithm previously applied to magnetization transfer and arterial spin labeling. The resulting optimal sampling schedule samples repeatedly around the resonance frequency of the amine pool and also near to the water resonance to maximize the information present within the data for quantitative model-based analysis. Simulation and experimental results on tissue-like phantoms showed that greater accuracy and precision (&gt;30% and &gt;46%, respectively, for some cases) were achieved in the parameters of interest when using optimal sampling schedule compared with evenly distributed sampling schedule. Hence, the proposed optimal sampling schedule could replace evenly distributed sampling schedule in chemical exchange saturation transfer imaging to improve the quantification of the chemical exchange saturation transfer effect and parameter estimation. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24600" xmlns="http://purl.org/rss/1.0/"><title>Model-based Acceleration of Parameter mapping (MAP) for saturation prepared radially acquired data</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24600</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Model-based Acceleration of Parameter mapping (MAP) for saturation prepared radially acquired data</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Johannes Tran-Gia, Daniel Stäb, Tobias Wech, Dietbert Hahn, Herbert Köstler</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-11T10:03:59.266917-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24600</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24600</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24600</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>A reconstruction technique called Model-based Acceleration of Parameter mapping (MAP) is presented allowing for quantification of longitudinal relaxation time and proton density from radial single-shot measurements after saturation recovery magnetization preparation. Using a mono-exponential model in image space, an iterative fitting algorithm is used to reconstruct one well resolved and consistent image for each of the projections acquired during the saturation recovery relaxation process. The functionality of the algorithm is examined in numerical simulations, phantom experiments, and in-vivo studies. MAP reconstructions of single-shot acquisitions feature the same image quality and resolution as fully sampled reference images in phantom and in-vivo studies. The longitudinal relaxation times obtained from the MAP reconstructions are in very good agreement with the reference values in numerical simulations as well as phantom and in-vivo measurements. Compared to available contrast manipulation techniques, no averaging of projections acquired at different time points of the relaxation process is required in MAP imaging. The proposed technique offers new ways of extracting quantitative information from single-shot measurements acquired after magnetization preparation. The reconstruction simultaneously yields images with high spatiotemporal resolution fully consistent with the acquired data as well as maps of the effective longitudinal relaxation parameter and the relative proton density. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.</p></div>
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A reconstruction technique called Model-based Acceleration of Parameter mapping (MAP) is presented allowing for quantification of longitudinal relaxation time and proton density from radial single-shot measurements after saturation recovery magnetization preparation. Using a mono-exponential model in image space, an iterative fitting algorithm is used to reconstruct one well resolved and consistent image for each of the projections acquired during the saturation recovery relaxation process. The functionality of the algorithm is examined in numerical simulations, phantom experiments, and in-vivo studies. MAP reconstructions of single-shot acquisitions feature the same image quality and resolution as fully sampled reference images in phantom and in-vivo studies. The longitudinal relaxation times obtained from the MAP reconstructions are in very good agreement with the reference values in numerical simulations as well as phantom and in-vivo measurements. Compared to available contrast manipulation techniques, no averaging of projections acquired at different time points of the relaxation process is required in MAP imaging. The proposed technique offers new ways of extracting quantitative information from single-shot measurements acquired after magnetization preparation. The reconstruction simultaneously yields images with high spatiotemporal resolution fully consistent with the acquired data as well as maps of the effective longitudinal relaxation parameter and the relative proton density. Magn Reson Med, 2013. © 2013 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24565" xmlns="http://purl.org/rss/1.0/"><title>Cine-ASL: A steady-pulsed arterial spin labeling method for myocardial perfusion mapping in mice. Part I. Experimental study</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24565</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cine-ASL: A steady-pulsed arterial spin labeling method for myocardial perfusion mapping in mice. Part I. Experimental study</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Thomas Troalen, Thibaut Capron, Patrick J. Cozzone, Monique Bernard, Frank Kober</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-01-02T12:40:56.411847-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24565</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24565</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24565</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Arterial spin labeling has been developed and used for the quantitative and completely noninvasive assessment of myocardial perfusion in vivo. Here we propose a novel arterial spin labeling method called cine-ASL, which is based on an electrocardiogram-gated steady-pulsed labeling approach combined with simultaneous readout over the cardiac cycle using cine-fast low-angle shot. This method led to shorter acquisition times than the previously used Look-Locker flow-sensitive alternating inversion recovery gradient-echo technique while preserving spatial resolution and robustness with respect to cardiac motion. High resolution perfusion mapping (in-plane resolution = 195 μm × 391 μm) was carried out with both techniques at 4.7 T in a group of 14 healthy mice. Mean perfusion values were 5.0 ± 0.8 mL g<sup>−1</sup> min<sup>−1</sup> with cine-ASL and 5.9 ± 1.4 mL g<sup>−1</sup> min<sup>−1</sup> with Look-Locker flow-sensitive alternating inversion recovery. In one animal, physiological stress was induced with higher anesthetic concentration to evaluate the response of both methods under vasodilation. Global myocardial perfusion increased from 5.6 to 16.0 mL g<sup>−1</sup> min<sup>−1</sup> with cine-ASL and from 6.3 to 18.7 mL g<sup>−1</sup> min<sup>−1</sup> with Look-Locker flow-sensitive alternating inversion recovery. Although this original scheme requires a separate <em>T</em><sub>1</sub> measurement to be fully quantitative, it improves arterial spin labeling sensitivity while maintaining compatibility with motion constraints in cardiac MRI in small rodents. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div>
]]></content:encoded><description>

Arterial spin labeling has been developed and used for the quantitative and completely noninvasive assessment of myocardial perfusion in vivo. Here we propose a novel arterial spin labeling method called cine-ASL, which is based on an electrocardiogram-gated steady-pulsed labeling approach combined with simultaneous readout over the cardiac cycle using cine-fast low-angle shot. This method led to shorter acquisition times than the previously used Look-Locker flow-sensitive alternating inversion recovery gradient-echo technique while preserving spatial resolution and robustness with respect to cardiac motion. High resolution perfusion mapping (in-plane resolution = 195 μm × 391 μm) was carried out with both techniques at 4.7 T in a group of 14 healthy mice. Mean perfusion values were 5.0 ± 0.8 mL g−1 min−1 with cine-ASL and 5.9 ± 1.4 mL g−1 min−1 with Look-Locker flow-sensitive alternating inversion recovery. In one animal, physiological stress was induced with higher anesthetic concentration to evaluate the response of both methods under vasodilation. Global myocardial perfusion increased from 5.6 to 16.0 mL g−1 min−1 with cine-ASL and from 6.3 to 18.7 mL g−1 min−1 with Look-Locker flow-sensitive alternating inversion recovery. Although this original scheme requires a separate T1 measurement to be fully quantitative, it improves arterial spin labeling sensitivity while maintaining compatibility with motion constraints in cardiac MRI in small rodents. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24569" xmlns="http://purl.org/rss/1.0/"><title>Improved first-pass spiral myocardial perfusion imaging with variable density trajectories</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24569</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Improved first-pass spiral myocardial perfusion imaging with variable density trajectories</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Michael Salerno, Christopher Sica, Christopher M. Kramer, Craig H. Meyer</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-27T13:42:33.070615-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24569</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24569</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24569</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>To develop and evaluate variable-density spiral first-pass perfusion pulse sequences for improved efficiency and off-resonance performance and to demonstrate the utility of an apodizing density compensation function (DCF) to improve signal-to-noise ratio (SNR) and reduce dark-rim artifact caused by cardiac motion and Gibbs Ringing.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>Three variable density spiral trajectories were designed, simulated, and evaluated in 18 normal subjects, and in eight patients with cardiac pathology on a 1.5T scanner.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>By using a DCF, which intentionally apodizes the <em>k</em>-space data, the sidelobe amplitude of the theoretical point spread function (PSF) is reduced by 68%, with only a 13% increase in the full-width at half-maximum of the main-lobe when compared with the same data corrected with a conventional variable-density DCF, and has an 8% higher resolution than a uniform density spiral with the same number of interleaves and readout duration. Furthermore, this strategy results in a greater than 60% increase in measured SNR when compared with the same variable-density spiral data corrected with a conventional DCF (<em>P</em> &lt; 0.01). Perfusion defects could be clearly visualized with minimal off-resonance and dark-rim artifacts.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>Variable-density spiral pulse sequences using an apodized DCF produce high-quality first-pass perfusion images with minimal dark-rim and off-resonance artifacts, high SNR and contrast-to-noise ratio, and good delineation of resting perfusion abnormalities. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
To develop and evaluate variable-density spiral first-pass perfusion pulse sequences for improved efficiency and off-resonance performance and to demonstrate the utility of an apodizing density compensation function (DCF) to improve signal-to-noise ratio (SNR) and reduce dark-rim artifact caused by cardiac motion and Gibbs Ringing.


Methods:
Three variable density spiral trajectories were designed, simulated, and evaluated in 18 normal subjects, and in eight patients with cardiac pathology on a 1.5T scanner.


Results:
By using a DCF, which intentionally apodizes the k-space data, the sidelobe amplitude of the theoretical point spread function (PSF) is reduced by 68%, with only a 13% increase in the full-width at half-maximum of the main-lobe when compared with the same data corrected with a conventional variable-density DCF, and has an 8% higher resolution than a uniform density spiral with the same number of interleaves and readout duration. Furthermore, this strategy results in a greater than 60% increase in measured SNR when compared with the same variable-density spiral data corrected with a conventional DCF (P &lt; 0.01). Perfusion defects could be clearly visualized with minimal off-resonance and dark-rim artifacts.


Conclusion:
Variable-density spiral pulse sequences using an apodized DCF produce high-quality first-pass perfusion images with minimal dark-rim and off-resonance artifacts, high SNR and contrast-to-noise ratio, and good delineation of resting perfusion abnormalities. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24579" xmlns="http://purl.org/rss/1.0/"><title>Turbo fast three-dimensional carotid artery black-blood MRI by combining three-dimensional MERGE sequence with compressed sensing</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24579</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Turbo fast three-dimensional carotid artery black-blood MRI by combining three-dimensional MERGE sequence with compressed sensing</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Bo Li, Li Dong, Bin Chen, Shuangxi Ji, Wenchao Cai, Ye Wang, Jue Zhang, Zhaoqi Zhang, Xiaoying Wang, Jing Fang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-27T13:42:26.673695-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24579</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24579</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24579</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4><b>Purpose:</b></h4><div class="para"><p>In this study, we sought to investigate the feasibility of turbo fast three-dimensional (3D) black-blood imaging by combining a 3D motion-sensitizing driven equilibrium rapid gradient echo sequence with compressed sensing.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4><b>Methods:</b></h4><div class="para"><p>A pseudo-centric phase encoding order was developed for compressed sensing-3D motion-sensitizing driven equilibrium rapid gradient echo to suppress flow signal in undersampled 3D k-space. Nine healthy volunteers were recruited for this study. Signal-to-tissue ratio, contrast-to-tissue ratio (CTR) and CTR efficiency (CTR<sub>eff</sub>) between fully sampled and undersampled images were calculated and compared in seven subjects. Moreover, isotropic high resolution images using different compressed sensing acceleration factors were evaluated in two other subjects.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4><b>Results:</b></h4><div class="para"><p>Wall-lumen signal-to-tissue ratio or CTR were comparable between the undersampled and the fully sampled images, while significant improvement of CTR<sub>eff</sub> was achieved in the undersampled images. At an isotropic high spatial resolution of 0.7 × 0.7 × 0.7 mm<sup>3</sup>, all undersampled images exhibited similar level of the flow suppression efficiency and the capability of delineating outer vessel wall boundary and lumen-wall interface, when compared with the fully sampled images.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4><b>Conclusion:</b></h4><div class="para"><p>The proposed turbo fast compressed sensing 3D black-blood imaging technique improves scan efficiency without sacrificing flow suppression efficiency and vessel wall image quality. It could be a valuable tool for rapid 3D vessel wall imaging. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
In this study, we sought to investigate the feasibility of turbo fast three-dimensional (3D) black-blood imaging by combining a 3D motion-sensitizing driven equilibrium rapid gradient echo sequence with compressed sensing.


Methods:
A pseudo-centric phase encoding order was developed for compressed sensing-3D motion-sensitizing driven equilibrium rapid gradient echo to suppress flow signal in undersampled 3D k-space. Nine healthy volunteers were recruited for this study. Signal-to-tissue ratio, contrast-to-tissue ratio (CTR) and CTR efficiency (CTReff) between fully sampled and undersampled images were calculated and compared in seven subjects. Moreover, isotropic high resolution images using different compressed sensing acceleration factors were evaluated in two other subjects.


Results:
Wall-lumen signal-to-tissue ratio or CTR were comparable between the undersampled and the fully sampled images, while significant improvement of CTReff was achieved in the undersampled images. At an isotropic high spatial resolution of 0.7 × 0.7 × 0.7 mm3, all undersampled images exhibited similar level of the flow suppression efficiency and the capability of delineating outer vessel wall boundary and lumen-wall interface, when compared with the fully sampled images.


Conclusion:
The proposed turbo fast compressed sensing 3D black-blood imaging technique improves scan efficiency without sacrificing flow suppression efficiency and vessel wall image quality. It could be a valuable tool for rapid 3D vessel wall imaging. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24581" xmlns="http://purl.org/rss/1.0/"><title>R1 and R2* changes in the human placenta in response to maternal oxygen challenge</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24581</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">R1 and R2* changes in the human placenta in response to maternal oxygen challenge</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Isaac Huen, David M. Morris, Caroline Wright, Geoff J. M. Parker, Colin P. Sibley, Edward D. Johnstone, Josephine H. Naish</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-27T13:42:19.057928-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24581</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24581</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24581</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>Pregnancy complications such as preeclampsia and fetal growth restriction are sometimes thought to be caused by placental abnormalities associated with reduced oxygenation. Oxygen-enhanced MRI (<em>R</em><sub>1</sub> contrast) and BOLD MRI (<em>R</em><sub>2</sub>* contrast) have the potential to noninvasively investigate this oxygen environment at a range of gestational ages.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>Scanning was carried out at 1.5 T under maternal air and oxygen breathing in a single placental slice in 14 healthy pregnant subjects of gestational ages 21–37 weeks. We report <em>R</em><sub>1</sub> changes using a respiratory-triggered inversion recovery-turbo spin-echo sequence, which is sensitive to changes in PO<sub>2</sub>, and <em>R</em><sub>2</sub>* changes using a breathhold multiple gradient-recalled echo sequence sensitive to changes in oxygen saturation.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>Significant <em>R</em><sub>1</sub> increases (<em>P</em> &lt; 0.005, paired t-test) and <em>R</em><sub>2</sub>* decreases (<em>P</em> &lt; 0.0001, paired t-test) between air and oxygen breathing were demonstrated. Δ<em>R</em><sub>1</sub> decreased with gestational age (<em>P</em> &lt; 0.0005, <em>r</em> = −0.835, Pearson correlation test). No significant effect of gestational age on <em>R</em><sub>2</sub>* change was observed.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>The results demonstrate the feasibility of non-invasive investigation of placental oxygenation using MRI and the sensitivity of <em>R</em><sub>1</sub> oxygen-enhanced MRI to gestational age. The techniques have the potential to provide unique noninvasive biomarkers in compromised pregnancies. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
Pregnancy complications such as preeclampsia and fetal growth restriction are sometimes thought to be caused by placental abnormalities associated with reduced oxygenation. Oxygen-enhanced MRI (R1 contrast) and BOLD MRI (R2* contrast) have the potential to noninvasively investigate this oxygen environment at a range of gestational ages.


Methods:
Scanning was carried out at 1.5 T under maternal air and oxygen breathing in a single placental slice in 14 healthy pregnant subjects of gestational ages 21–37 weeks. We report R1 changes using a respiratory-triggered inversion recovery-turbo spin-echo sequence, which is sensitive to changes in PO2, and R2* changes using a breathhold multiple gradient-recalled echo sequence sensitive to changes in oxygen saturation.


Results:
Significant R1 increases (P &lt; 0.005, paired t-test) and R2* decreases (P &lt; 0.0001, paired t-test) between air and oxygen breathing were demonstrated. ΔR1 decreased with gestational age (P &lt; 0.0005, r = −0.835, Pearson correlation test). No significant effect of gestational age on R2* change was observed.


Conclusion:
The results demonstrate the feasibility of non-invasive investigation of placental oxygenation using MRI and the sensitivity of R1 oxygen-enhanced MRI to gestational age. The techniques have the potential to provide unique noninvasive biomarkers in compromised pregnancies. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24586" xmlns="http://purl.org/rss/1.0/"><title>Arrhythmia insensitive rapid cardiac T1 mapping pulse sequence</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24586</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Arrhythmia insensitive rapid cardiac T1 mapping pulse sequence</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Michelle Fitts, Elodie Breton, Eugene G. Kholmovski, Derek J. Dosdall, Sathya Vijayakumar, Kyung P. Hong, Ravi Ranjan, Nassir F. Marrouche, Leon Axel, Daniel Kim</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-27T13:41:58.567212-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24586</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24586</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24586</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>To develop an arrhythmia-insensitive rapid (AIR) cardiac <em>T</em><sub>1</sub> mapping pulse sequence for quantification of diffuse fibrosis.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>An arrhythmia-insensitive cardiac <em>T</em><sub>1</sub> mapping pulse sequence was developed based on saturation recovery <em>T</em><sub>1</sub> weighting, which is inherently insensitive to heart rate and rhythm, and two single-shot balanced steady-state free precession image acquisitions with centric k-space ordering, where <em>T</em><sub>1</sub> calculation is inherently insensitive to <em>T</em><sub>2</sub> effects. Its performance against conventional cardiac <em>T</em><sub>1</sub> mapping based on inversion recovery (i.e., MOLLI) is compared. Phantom experiments (<em>T</em><sub>1</sub> ranging from 535 to 2123 ms) were performed with heart rate and rhythm simulated at 60 and 120 beats per minute (bpm) and arrhythmia using an external triggering device. Ten human subjects and 17 large animals were scanned precontrast and 5, 10, and 15 min after contrast agent administration.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>Compared with the reference <em>T</em><sub>1</sub> mapping, AIR yielded lower normalized root-mean-square error than MOLLI (8% vs. 3%, respectively, at 60 bpm, 28% vs. 3%, respectively, at 120 bpm, and 22% vs. 3%, respectively, at arrhythmia). In vivo studies showed that <em>T</em><sub>1</sub> measurements made by MOLLI and AIR were strongly correlated (<em>r</em> = 0.99) but in poor agreement (mean difference = 161.8 ms, upper and lower 95% limits of agreements = 347.5 ms and −24.0 ms).</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>Our AIR pulse sequence may be clinically useful for assessment of diffuse myocardial fibrosis in patients. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
To develop an arrhythmia-insensitive rapid (AIR) cardiac T1 mapping pulse sequence for quantification of diffuse fibrosis.


Methods:
An arrhythmia-insensitive cardiac T1 mapping pulse sequence was developed based on saturation recovery T1 weighting, which is inherently insensitive to heart rate and rhythm, and two single-shot balanced steady-state free precession image acquisitions with centric k-space ordering, where T1 calculation is inherently insensitive to T2 effects. Its performance against conventional cardiac T1 mapping based on inversion recovery (i.e., MOLLI) is compared. Phantom experiments (T1 ranging from 535 to 2123 ms) were performed with heart rate and rhythm simulated at 60 and 120 beats per minute (bpm) and arrhythmia using an external triggering device. Ten human subjects and 17 large animals were scanned precontrast and 5, 10, and 15 min after contrast agent administration.


Results:
Compared with the reference T1 mapping, AIR yielded lower normalized root-mean-square error than MOLLI (8% vs. 3%, respectively, at 60 bpm, 28% vs. 3%, respectively, at 120 bpm, and 22% vs. 3%, respectively, at arrhythmia). In vivo studies showed that T1 measurements made by MOLLI and AIR were strongly correlated (r = 0.99) but in poor agreement (mean difference = 161.8 ms, upper and lower 95% limits of agreements = 347.5 ms and −24.0 ms).


Conclusion:
Our AIR pulse sequence may be clinically useful for assessment of diffuse myocardial fibrosis in patients. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24590" xmlns="http://purl.org/rss/1.0/"><title>Pattern analysis accounts for heterogeneity observed in MRI studies of tumor angiogenesis</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24590</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Pattern analysis accounts for heterogeneity observed in MRI studies of tumor angiogenesis</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Marco Dominietto, Steffi Lehmann, Ruth Keist, Markus Rudin</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-27T13:41:23.422532-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24590</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24590</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24590</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>MRI is a method of choice for assessing anatomical structures or angiogenesis-related parameters noninvasively during tumor progression. Typically, tumor tissue displays a high degree of heterogeneity that can be evaluated using pattern analysis (PA), which comprises shape and texture analysis. This work aims at implementing PA methods to study angiogenesis in a murine tumor model and testing its sensitivity with regard to detecting changes elicited by administration of a drug. Twelve balb/c-nude mice were injected subcutaneously with 10<sup>6</sup> C51 cells (colon carcinoma). A first group (<em>N</em> = 6) of animals was treated with dimethyloxalylglycine, a drug known to stabilize hypoxia-inducible-factor-α, which among other functions, is involved in angiogenesis. The second group (<em>N</em> = 6) was treated with saline. MRI experiments assessing tumor blood volume and permeability-maps (<em>K</em><sup>trans</sup>) were performed immediately before and 6 days after drug treatment. Data have been analyzed using standard histogram analysis and PA. Standard histogram analysis did not reveal any difference between the two groups, neither before nor after the treatment. In contrast, PA revealed significant differences between drug and placebo treated mice in the texture of the TBV and <em>K</em><sup>trans</sup> maps after drug treatment, but not with regard to tumors shapes. The results indicated that in view of the heterogeneity of tumor tissue, standard histogram analysis appears insensitive in picking-up differences in response to treatment, while PA appears to be particularly sensitive to changes in texture. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div>
]]></content:encoded><description>

MRI is a method of choice for assessing anatomical structures or angiogenesis-related parameters noninvasively during tumor progression. Typically, tumor tissue displays a high degree of heterogeneity that can be evaluated using pattern analysis (PA), which comprises shape and texture analysis. This work aims at implementing PA methods to study angiogenesis in a murine tumor model and testing its sensitivity with regard to detecting changes elicited by administration of a drug. Twelve balb/c-nude mice were injected subcutaneously with 106 C51 cells (colon carcinoma). A first group (N = 6) of animals was treated with dimethyloxalylglycine, a drug known to stabilize hypoxia-inducible-factor-α, which among other functions, is involved in angiogenesis. The second group (N = 6) was treated with saline. MRI experiments assessing tumor blood volume and permeability-maps (Ktrans) were performed immediately before and 6 days after drug treatment. Data have been analyzed using standard histogram analysis and PA. Standard histogram analysis did not reveal any difference between the two groups, neither before nor after the treatment. In contrast, PA revealed significant differences between drug and placebo treated mice in the texture of the TBV and Ktrans maps after drug treatment, but not with regard to tumors shapes. The results indicated that in view of the heterogeneity of tumor tissue, standard histogram analysis appears insensitive in picking-up differences in response to treatment, while PA appears to be particularly sensitive to changes in texture. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24601" xmlns="http://purl.org/rss/1.0/"><title>Partial volume correction in arterial spin labeling using a Look-Locker sequence</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24601</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Partial volume correction in arterial spin labeling using a Look-Locker sequence</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Jan Petr, Georg Schramm, Frank Hofheinz, Jens Langner, Jörg van den Hoff</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-27T13:41:09.603054-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24601</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24601</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24601</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>Partial volume (PV) effects are caused by limited spatial resolution and significantly affect cerebral blood flow investigations with arterial spin labeling. Therefore, accurate PV correction (PVC) procedures are required. PVC is commonly based on PV maps obtained from segmented high-resolution <em>T</em><sub>1</sub>-weighted images. Segmentation of these images is error-prone, and it can be difficult to coregister these images accurately with the single-shot ASL images such as those created by echo-planar imaging (EPI). In this paper, an alternative method for PV map generation is proposed.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>The Look-Locker EPI (LL-EPI) acquisition is used for analyzing the <em>T</em><sub>1</sub>-recovery curve and for subsequent PV map generation. The new method was evaluated in five healthy volunteers (mean age 30 ± 3.7 years).</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>By applying a linear regression method for PVC, a 12% decrease in regression error was reached with the new method.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>PV maps extraction from LL-EPI is a viable, possibly superior alternative to the standard approach based on segmentation of high-resolution <em>T</em><sub>1</sub>-weighted images. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
Partial volume (PV) effects are caused by limited spatial resolution and significantly affect cerebral blood flow investigations with arterial spin labeling. Therefore, accurate PV correction (PVC) procedures are required. PVC is commonly based on PV maps obtained from segmented high-resolution T1-weighted images. Segmentation of these images is error-prone, and it can be difficult to coregister these images accurately with the single-shot ASL images such as those created by echo-planar imaging (EPI). In this paper, an alternative method for PV map generation is proposed.


Methods:
The Look-Locker EPI (LL-EPI) acquisition is used for analyzing the T1-recovery curve and for subsequent PV map generation. The new method was evaluated in five healthy volunteers (mean age 30 ± 3.7 years).


Results:
By applying a linear regression method for PVC, a 12% decrease in regression error was reached with the new method.


Conclusion:
PV maps extraction from LL-EPI is a viable, possibly superior alternative to the standard approach based on segmentation of high-resolution T1-weighted images. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24563" xmlns="http://purl.org/rss/1.0/"><title>Error model for reduction of cardiac and respiratory motion effects in quantitative liver DW-MRI</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24563</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Error model for reduction of cardiac and respiratory motion effects in quantitative liver DW-MRI</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Paul Murphy, Tanya Wolfson, Anthony Gamst, Claude Sirlin, Mark Bydder</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-27T13:41:02.079923-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24563</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24563</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24563</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>Diffusion-weighted images of the liver exhibit signal dropout from cardiac and respiratory motion, particularly in the left lobe. These artifacts cause bias and variance in derived parameters that quantify intravoxel incoherent motion. Many models of diffusion have been proposed, but few separate attenuation from diffusion or perfusion from that of bulk motion. The error model proposed here (Beta*LogNormal) is intended to accomplish that separation by modeling stochastic attenuation from bulk motion as multiplication by a Beta-distributed random variate. Maximum likelihood estimation with this error model can be used to derive intravoxel incoherent motion parameters separate from signal dropout, and does not require a priori specification of parameters to do so. Liver intravoxel incoherent motion parameters were derived for six healthy subjects under this error model and compared with least-squares estimates. Least-squares estimates exhibited bias due to cardiac and respiratory gating and due to location within the liver. Bias from these factors was significantly reduced under the Beta*LogNormal model, as was within-organ parameter variance. Similar effects were appreciable in diffusivity maps in two patients with focal liver lesions. These results suggest that, relative to least-squares estimation, the Beta*LogNormal model accomplishes the intended reduction of bias and variance from bulk motion in liver diffusion imaging. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div>
]]></content:encoded><description>

Diffusion-weighted images of the liver exhibit signal dropout from cardiac and respiratory motion, particularly in the left lobe. These artifacts cause bias and variance in derived parameters that quantify intravoxel incoherent motion. Many models of diffusion have been proposed, but few separate attenuation from diffusion or perfusion from that of bulk motion. The error model proposed here (Beta*LogNormal) is intended to accomplish that separation by modeling stochastic attenuation from bulk motion as multiplication by a Beta-distributed random variate. Maximum likelihood estimation with this error model can be used to derive intravoxel incoherent motion parameters separate from signal dropout, and does not require a priori specification of parameters to do so. Liver intravoxel incoherent motion parameters were derived for six healthy subjects under this error model and compared with least-squares estimates. Least-squares estimates exhibited bias due to cardiac and respiratory gating and due to location within the liver. Bias from these factors was significantly reduced under the Beta*LogNormal model, as was within-organ parameter variance. Similar effects were appreciable in diffusivity maps in two patients with focal liver lesions. These results suggest that, relative to least-squares estimation, the Beta*LogNormal model accomplishes the intended reduction of bias and variance from bulk motion in liver diffusion imaging. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24587" xmlns="http://purl.org/rss/1.0/"><title>Perfusion quantification by model-free arterial spin labeling using nonlinear stochastic regularization deconvolution</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24587</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Perfusion quantification by model-free arterial spin labeling using nonlinear stochastic regularization deconvolution</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">André Ahlgren, Ronnie Wirestam, Esben Thade Petersen, Freddy Ståhlberg, Linda Knutsson</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-27T13:40:54.960261-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24587</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24587</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24587</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-0" xmlns="http://www.w3.org/1999/xhtml"><div class="para"><p><b>Purpose</b>: Quantification of cerebral blood flow can be accomplished by model-free arterial spin labeling using the quantitative STAR labeling of arterial regions (QUASAR) sequence. The required deconvolution is normally based on block-circulant singular value decomposition (cSVD)/oscillation SVD (oSVD), an algorithm associated with nonphysiological residue functions and potential effects of arterial dispersion. The aim of this work was to amend this by implementing nonlinear stochastic regularization (NSR) deconvolution, previously used to retrieve realistic residue functions in dynamic susceptibility contrast MRI.</p></div></div>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>To characterize the residue function in model-free arterial spin labeling, and possibly to improve absolute cerebral blood flow quantification, NSR was applied to deconvolution of QUASAR data. For comparison, SVD-based deconvolution was also employed. Residue function characteristics and cerebral blood flow values from 10 volunteers were obtained. Simulations were performed to support the in vivo results.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>NSR was able to resolve realistic residue functions in contrast to the SVD-based methods. Mean cerebral blood flow estimates in gray matter were 36.6 ± 2.6, 28.6 ± 3.3, 40.9 ± 3.6, and 42.9 ± 3.9 mL/100 g/min for cSVD, oSVD, NSR, and NSR with correction for arterial dispersion, respectively. In simulations, the NSR-based perfusion estimates showed better accuracy than the SVD-based approaches.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>Perfusion quantification by model-free arterial spin labeling is evidently dependent on the selected deconvolution method, and NSR is a feasible alternative to SVD-based methods. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose: Quantification of cerebral blood flow can be accomplished by model-free arterial spin labeling using the quantitative STAR labeling of arterial regions (QUASAR) sequence. The required deconvolution is normally based on block-circulant singular value decomposition (cSVD)/oscillation SVD (oSVD), an algorithm associated with nonphysiological residue functions and potential effects of arterial dispersion. The aim of this work was to amend this by implementing nonlinear stochastic regularization (NSR) deconvolution, previously used to retrieve realistic residue functions in dynamic susceptibility contrast MRI.


Methods:
To characterize the residue function in model-free arterial spin labeling, and possibly to improve absolute cerebral blood flow quantification, NSR was applied to deconvolution of QUASAR data. For comparison, SVD-based deconvolution was also employed. Residue function characteristics and cerebral blood flow values from 10 volunteers were obtained. Simulations were performed to support the in vivo results.


Results:
NSR was able to resolve realistic residue functions in contrast to the SVD-based methods. Mean cerebral blood flow estimates in gray matter were 36.6 ± 2.6, 28.6 ± 3.3, 40.9 ± 3.6, and 42.9 ± 3.9 mL/100 g/min for cSVD, oSVD, NSR, and NSR with correction for arterial dispersion, respectively. In simulations, the NSR-based perfusion estimates showed better accuracy than the SVD-based approaches.


Conclusion:
Perfusion quantification by model-free arterial spin labeling is evidently dependent on the selected deconvolution method, and NSR is a feasible alternative to SVD-based methods. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24588" xmlns="http://purl.org/rss/1.0/"><title>Cine-ASL: A steady-pulsed arterial spin labeling method for myocardial perfusion mapping in mice. Part II. Theoretical model and sensitivity optimization</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24588</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cine-ASL: A steady-pulsed arterial spin labeling method for myocardial perfusion mapping in mice. Part II. Theoretical model and sensitivity optimization</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Thibaut Capron, Thomas Troalen, Patrick J. Cozzone, Monique Bernard, Frank Kober</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-27T13:40:47.354594-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24588</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24588</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24588</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>In small rodent myocardial perfusion studies, the most widely used method is based on Look-Locker measurements of the magnetization recovery after FAIR preparation, which bears limitations regarding acquisition efficiency due to the pulsed arterial spin labeling nature of the sequence. To improve efficiency, this two-article set proposes a new steady-pulsed arterial spin labeling scheme using a cine readout incorporating one tagging pulse per heart cycle. In this part, we derive a theoretical description of the magnetization time evolution in such a scheme. The combination of steady-pulsed labeling and cine readout drives tissue magnetization into a stationary regime that explicitly depends on perfusion. In comparison with dedicated experiments on the mouse heart, the model is discussed and validated for perfusion quantification. The model predicts that in this regime, signal is independent of irregular dynamics occurring during acquisition, such as heart rate variations or arterial input function. Optimization of the sequence offers the possibility to increase the signal to noise ratio by efficient signal averaging. The sensitivity of this new method is shown to be more than three times larger than previously used techniques. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div>
]]></content:encoded><description>

In small rodent myocardial perfusion studies, the most widely used method is based on Look-Locker measurements of the magnetization recovery after FAIR preparation, which bears limitations regarding acquisition efficiency due to the pulsed arterial spin labeling nature of the sequence. To improve efficiency, this two-article set proposes a new steady-pulsed arterial spin labeling scheme using a cine readout incorporating one tagging pulse per heart cycle. In this part, we derive a theoretical description of the magnetization time evolution in such a scheme. The combination of steady-pulsed labeling and cine readout drives tissue magnetization into a stationary regime that explicitly depends on perfusion. In comparison with dedicated experiments on the mouse heart, the model is discussed and validated for perfusion quantification. The model predicts that in this regime, signal is independent of irregular dynamics occurring during acquisition, such as heart rate variations or arterial input function. Optimization of the sequence offers the possibility to increase the signal to noise ratio by efficient signal averaging. The sensitivity of this new method is shown to be more than three times larger than previously used techniques. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24591" xmlns="http://purl.org/rss/1.0/"><title>Spin echo measurements of the extravasation and tumor cell uptake of hyperpolarized [1-13C]lactate and [1-13C]pyruvate</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24591</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Spin echo measurements of the extravasation and tumor cell uptake of hyperpolarized [1-13C]lactate and [1-13C]pyruvate</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mikko I. Kettunen, Brett W. C. Kennedy, De-en Hu, Kevin M. Brindle</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-27T13:40:39.624341-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24591</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24591</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24591</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>To assess the blood-tissue distribution of hyperpolarized <sup>13</sup>C-labeled molecules in vivo.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>Spin-echo experiments with simultaneous acquisition of the free induction decay (FID) signal following the excitation pulse and the spin-echo signal, were used to monitor hyperpolarized [1-<sup>13</sup>C]lactate, [1-<sup>13</sup>C]pyruvate, and the perfusion marker, [<sup>13</sup>C]HP001, following their intravenous injection into tumor-bearing mice. Apparent <em>T</em><sub>2</sub> relaxation times and diffusion coefficients were also measured.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>An increasing tumor echo/FID ratio was observed for all three molecules, which could be explained by their extravasation into the tumor interstitial space, where <em>T</em><sub>2</sub> relaxation times were longer and diffusion coefficients smaller. Inhibition of the monocarboxylate transporter, which decreased by 40% the label exchange between pyruvate and lactate, reduced the increase in the echo/FID ratio for pyruvate and lactate, but not for HP001, demonstrating that some of the increase in the echo/FID ratio was due to cell uptake of lactate and pyruvate. The different relaxation and diffusion behavior of the intravascular and extravascular signals affected measurements of the apparent label exchange rate constants.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>Simultaneous collection of both FID and echo signals can provide information on cell uptake thus giving further insight into the kinetics of hyperpolarized <sup>13</sup>C label exchange. Care is needed when comparing exchange rate constants determined in spin-echo-based studies. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
To assess the blood-tissue distribution of hyperpolarized 13C-labeled molecules in vivo.


Methods:
Spin-echo experiments with simultaneous acquisition of the free induction decay (FID) signal following the excitation pulse and the spin-echo signal, were used to monitor hyperpolarized [1-13C]lactate, [1-13C]pyruvate, and the perfusion marker, [13C]HP001, following their intravenous injection into tumor-bearing mice. Apparent T2 relaxation times and diffusion coefficients were also measured.


Results:
An increasing tumor echo/FID ratio was observed for all three molecules, which could be explained by their extravasation into the tumor interstitial space, where T2 relaxation times were longer and diffusion coefficients smaller. Inhibition of the monocarboxylate transporter, which decreased by 40% the label exchange between pyruvate and lactate, reduced the increase in the echo/FID ratio for pyruvate and lactate, but not for HP001, demonstrating that some of the increase in the echo/FID ratio was due to cell uptake of lactate and pyruvate. The different relaxation and diffusion behavior of the intravascular and extravascular signals affected measurements of the apparent label exchange rate constants.


Conclusion:
Simultaneous collection of both FID and echo signals can provide information on cell uptake thus giving further insight into the kinetics of hyperpolarized 13C label exchange. Care is needed when comparing exchange rate constants determined in spin-echo-based studies. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24592" xmlns="http://purl.org/rss/1.0/"><title>High-frequency subband compressed sensing MRI using quadruplet sampling</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24592</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High-frequency subband compressed sensing MRI using quadruplet sampling</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Kyunghyun Sung, Brian A. Hargreaves</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-27T13:40:30.22408-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24592</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24592</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24592</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>To present and validate a new method that formalizes a direct link between k-space and wavelet domains to apply separate undersampling and reconstruction for high- and low-spatial-frequency k-space data.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Theory and Methods:</h4><div class="para"><p>High- and low-spatial-frequency regions are defined in k-space based on the separation of wavelet subbands, and the conventional compressed sensing problem is transformed into one of localized k-space estimation. To better exploit wavelet-domain sparsity, compressed sensing can be used for high-spatial-frequency regions, whereas parallel imaging can be used for low-spatial-frequency regions. Fourier undersampling is also customized to better accommodate each reconstruction method: random undersampling for compressed sensing and regular undersampling for parallel imaging.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>Examples using the proposed method demonstrate successful reconstruction of both low-spatial-frequency content and fine structures in high-resolution three-dimensional breast imaging with a net acceleration of 11–12.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>The proposed method improves the reconstruction accuracy of high-spatial-frequency signal content and avoids incoherent artifacts in low-spatial-frequency regions. This new formulation also reduces the reconstruction time due to the smaller problem size. <b>Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>


Purpose:
To present and validate a new method that formalizes a direct link between k-space and wavelet domains to apply separate undersampling and reconstruction for high- and low-spatial-frequency k-space data.


Theory and Methods:
High- and low-spatial-frequency regions are defined in k-space based on the separation of wavelet subbands, and the conventional compressed sensing problem is transformed into one of localized k-space estimation. To better exploit wavelet-domain sparsity, compressed sensing can be used for high-spatial-frequency regions, whereas parallel imaging can be used for low-spatial-frequency regions. Fourier undersampling is also customized to better accommodate each reconstruction method: random undersampling for compressed sensing and regular undersampling for parallel imaging.


Results:
Examples using the proposed method demonstrate successful reconstruction of both low-spatial-frequency content and fine structures in high-resolution three-dimensional breast imaging with a net acceleration of 11–12.


Conclusion:
The proposed method improves the reconstruction accuracy of high-spatial-frequency signal content and avoids incoherent artifacts in low-spatial-frequency regions. This new formulation also reduces the reconstruction time due to the smaller problem size. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24560" xmlns="http://purl.org/rss/1.0/"><title>Quantitative characterization of nuclear Overhauser enhancement and amide proton transfer effects in the human brain at 7 tesla</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24560</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Quantitative characterization of nuclear Overhauser enhancement and amide proton transfer effects in the human brain at 7 tesla</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Dapeng Liu, Jinyuan Zhou, Rong Xue, Zhentao Zuo, Jing An, Danny J. J. Wang</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-13T09:10:31.05819-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24560</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24560</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24560</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>This study aimed to quantitatively investigate two main magnetization transfer effects at low <em>B</em><sub>1</sub>: the nuclear Overhauser enhancement (NOE) and amide proton transfer in the human brain at 7 T.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>The magnetization transfer effects in the human brain were characterized using a four-pool proton model, which consisted of bulk water, macromolecules, an amide group of mobile proteins and peptides, and NOE-related protons resonating upfield. The pool sizes, exchange rates, and relaxation times of these proton pools were investigated quantitatively by fitting, and the net signals of amide proton transfer and NOE were simulated based on the fitted parameters.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>The results showed that the four-pool model fitted the experimental data quite well, and the NOE effects in human brain at 7 T had a broad spectrum distribution. The NOE effects peaked at a <em>B</em><sub>1</sub> of ∼ 1–1.4 μT and were significantly stronger in the white matter than in the gray matter, corresponding to a pool-size ratio ∼ 2:1. As the amide proton transfer effect was relatively small compared with the NOE effects, magnetization transfer asymmetry analysis yielded an NOE-dominated contrast in the healthy human brain in this range of <em>B</em><sub>1</sub>.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>These findings are important to identify the source of NOE effects and to quantify amide proton transfer effects in human brain at 7 T. <b>Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</b></p></div></div>
]]></content:encoded><description>


Purpose:
This study aimed to quantitatively investigate two main magnetization transfer effects at low B1: the nuclear Overhauser enhancement (NOE) and amide proton transfer in the human brain at 7 T.


Methods:
The magnetization transfer effects in the human brain were characterized using a four-pool proton model, which consisted of bulk water, macromolecules, an amide group of mobile proteins and peptides, and NOE-related protons resonating upfield. The pool sizes, exchange rates, and relaxation times of these proton pools were investigated quantitatively by fitting, and the net signals of amide proton transfer and NOE were simulated based on the fitted parameters.


Results:
The results showed that the four-pool model fitted the experimental data quite well, and the NOE effects in human brain at 7 T had a broad spectrum distribution. The NOE effects peaked at a B1 of ∼ 1–1.4 μT and were significantly stronger in the white matter than in the gray matter, corresponding to a pool-size ratio ∼ 2:1. As the amide proton transfer effect was relatively small compared with the NOE effects, magnetization transfer asymmetry analysis yielded an NOE-dominated contrast in the healthy human brain in this range of B1.


Conclusion:
These findings are important to identify the source of NOE effects and to quantify amide proton transfer effects in human brain at 7 T. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24566" xmlns="http://purl.org/rss/1.0/"><title>Utility of respiratory-navigator-rejected k-space lines for improved signal-to-noise ratio in three-dimensional cardiac MR</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24566</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Utility of respiratory-navigator-rejected k-space lines for improved signal-to-noise ratio in three-dimensional cardiac MR</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mehmet Akçakaya, Jaime L. Shaw, Thomas H. Hauser, Reza Nezafat</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-11T12:22:29.650061-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24566</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24566</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24566</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>To develop and evaluate a technique that uses the k-space lines rejected by prospective respiratory navigator (NAV) to improve the signal-to-noise ratio (SNR) without increasing the scan time.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>In conventional image reconstruction, the motion-corrupted k-space lines rejected by the NAV are not used. In this study, a set of translational motion parameters for the NAV-rejected lines and a phase-corrected average for the k-space line are estimated jointly using a maximum-likelihood approach and the information from the corresponding accepted k-space lines. Left coronary artery images were acquired in 10 healthy adult subjects, and the proposed approach incorporating the NAV-rejected lines was compared with the conventional dataset with NAV-accepted lines only, as well as a simple average of all k-space lines, in terms of SNR, normalized vessel sharpness and qualitative image scores on a four-point scale (1 = poor, 4 = excellent). Late gadolinium enhancement images of the left atrium were also acquired in 21 patients with atrial fibrillation pre- or post-pulmonary vein isolation. Images reconstructed with the proposed, conventional, and simple averaging methods were compared in terms of SNR, and subjective image quality on a four-point scale.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>For coronary MRI, there was a significant improvement in SNR with the proposed technique, but no significant difference in normalized vessel sharpness or qualitative image scores were observed with respect to the conventional method. Simple averaging resulted in an SNR gain, but significant loss in vessel sharpness and image quality. For late gadolinium enhancement, there was a significant increase in SNR, but no significant differences were observed in subjective image quality scores between the proposed and conventional methods. There was an SNR gain, but image quality loss for simple averaging, when compared with the conventional technique. In both coronary MRI and late gadolinium enhancement, the SNR gain of the proposed method was not significantly different than the maximum theoretical SNR gain.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>The proposed technique improves SNR using the additional information from NAV-rejected k-space lines, while providing similar image quality to standard reconstruction using motion-free k-space data only, with no increase in scan time. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
To develop and evaluate a technique that uses the k-space lines rejected by prospective respiratory navigator (NAV) to improve the signal-to-noise ratio (SNR) without increasing the scan time.


Methods:
In conventional image reconstruction, the motion-corrupted k-space lines rejected by the NAV are not used. In this study, a set of translational motion parameters for the NAV-rejected lines and a phase-corrected average for the k-space line are estimated jointly using a maximum-likelihood approach and the information from the corresponding accepted k-space lines. Left coronary artery images were acquired in 10 healthy adult subjects, and the proposed approach incorporating the NAV-rejected lines was compared with the conventional dataset with NAV-accepted lines only, as well as a simple average of all k-space lines, in terms of SNR, normalized vessel sharpness and qualitative image scores on a four-point scale (1 = poor, 4 = excellent). Late gadolinium enhancement images of the left atrium were also acquired in 21 patients with atrial fibrillation pre- or post-pulmonary vein isolation. Images reconstructed with the proposed, conventional, and simple averaging methods were compared in terms of SNR, and subjective image quality on a four-point scale.


Results:
For coronary MRI, there was a significant improvement in SNR with the proposed technique, but no significant difference in normalized vessel sharpness or qualitative image scores were observed with respect to the conventional method. Simple averaging resulted in an SNR gain, but significant loss in vessel sharpness and image quality. For late gadolinium enhancement, there was a significant increase in SNR, but no significant differences were observed in subjective image quality scores between the proposed and conventional methods. There was an SNR gain, but image quality loss for simple averaging, when compared with the conventional technique. In both coronary MRI and late gadolinium enhancement, the SNR gain of the proposed method was not significantly different than the maximum theoretical SNR gain.


Conclusion:
The proposed technique improves SNR using the additional information from NAV-rejected k-space lines, while providing similar image quality to standard reconstruction using motion-free k-space data only, with no increase in scan time. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24571" xmlns="http://purl.org/rss/1.0/"><title>Characterizing inter-compartmental water exchange in myelinated tissue using relaxation exchange spectroscopy</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24571</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Characterizing inter-compartmental water exchange in myelinated tissue using relaxation exchange spectroscopy</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Richard D. Dortch, Kevin D. Harkins, Meher R. Juttukonda, John C. Gore, Mark D. Does</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-11T12:21:54.357479-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24571</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24571</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24571</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Full Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p><b>Purpose</b>: To investigate inter-compartmental water exchange in two model myelinated tissues ex vivo using relaxation exchange spectroscopy. <b>Methods</b>: Building upon a previously developed theoretical framework, a three-compartment (myelin, intra-axonal, and extra-axonal water) model of the inversion-recovery prepared relaxation exchange spectroscopy signal was applied in excised rat optic nerve and frog sciatic nerve samples to estimate the water residence time constants in myelin (τ<sub>myelin</sub>). <b>Results</b>: In the rat optic nerve samples, τ<sub>myelin</sub> = 138 ± 15 ms (mean ± standard deviation) was estimated. In sciatic nerve, which possesses thicker myelin sheaths than optic nerve, a much longer τ<sub>myelin</sub> = 2046 ± 140 ms was observed. <b>Conclusions</b>: Consistent with previous studies in rat spinal cord, the extrapolation of exchange rates in optic nerve to in vivo conditions indicates that τ<sub>myelin</sub> &lt; 100 ms. This suggests that there is a significant effect of inter-compartmental water exchange on the transverse relaxation of water protons in white matter. The much longer τ<sub>myelin</sub> values in sciatic nerve supports the postulate that the inter-compartmental water exchange rate is mediated by myelin thickness. Together, these findings point to the potential for MRI methods to probe variations in myelin thickness in white matter. <b>Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.</b></p></div>
]]></content:encoded><description>

Purpose: To investigate inter-compartmental water exchange in two model myelinated tissues ex vivo using relaxation exchange spectroscopy. Methods: Building upon a previously developed theoretical framework, a three-compartment (myelin, intra-axonal, and extra-axonal water) model of the inversion-recovery prepared relaxation exchange spectroscopy signal was applied in excised rat optic nerve and frog sciatic nerve samples to estimate the water residence time constants in myelin (τmyelin). Results: In the rat optic nerve samples, τmyelin = 138 ± 15 ms (mean ± standard deviation) was estimated. In sciatic nerve, which possesses thicker myelin sheaths than optic nerve, a much longer τmyelin = 2046 ± 140 ms was observed. Conclusions: Consistent with previous studies in rat spinal cord, the extrapolation of exchange rates in optic nerve to in vivo conditions indicates that τmyelin &lt; 100 ms. This suggests that there is a significant effect of inter-compartmental water exchange on the transverse relaxation of water protons in white matter. The much longer τmyelin values in sciatic nerve supports the postulate that the inter-compartmental water exchange rate is mediated by myelin thickness. Together, these findings point to the potential for MRI methods to probe variations in myelin thickness in white matter. Magn Reson Med, 2012. © 2012 Wiley Periodicals, Inc.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24578" xmlns="http://purl.org/rss/1.0/"><title>High-resolution Fourier-encoded sub-millisecond echo time musculoskeletal imaging at 3 Tesla and 7 Tesla</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24578</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">High-resolution Fourier-encoded sub-millisecond echo time musculoskeletal imaging at 3 Tesla and 7 Tesla</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">X. Deligianni, P. Bär, K. Scheffler, S. Trattnig, O. Bieri</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2012-12-11T12:21:30.764387-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/mrm.24578</dc:identifier><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc.</dc:publisher><prism:doi xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">10.1002/mrm.24578</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24578</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Note</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">n/a</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[
<h3 xhtml="http://www.w3.org/1999/xhtml" xmlns:ol="http://www.wiley.com/namespaces/ol/xsl-lib">Abstract</h3>
<div class="section" id="abs1-1" xmlns="http://www.w3.org/1999/xhtml"><h4>Purpose:</h4><div class="para"><p>The feasibility of imaging musculoskeletal fibrous tissue components, such as menisci, ligaments, and tendons, with a conventional spoiled gradient echo technique is explored in vivo at 3 T and 7 T.</p></div></div>
<div class="section" id="abs1-2" xmlns="http://www.w3.org/1999/xhtml"><h4>Methods:</h4><div class="para"><p>To this end, the echo time (TE<sub>1</sub>) of a conventional Fourier-encoded multicontrast three-dimensional SGPR sequence is minimized by using nonselective excitation pulses, highly asymmetric readouts, and a variable TE<sub>1</sub> along the phase and slice encoding direction. In addition, a fully sampled second echo image (with TE<sub>2</sub> &gt;&gt; TE<sub>1</sub>) can be used to highlight components with short transverse relaxation times in a difference image with positive contrast.</p></div></div>
<div class="section" id="abs1-3" xmlns="http://www.w3.org/1999/xhtml"><h4>Results:</h4><div class="para"><p>Fourier-encoded spoiled gradient echo sequences are able to provide sub-millisecond TE<sub>1</sub> of about 800 μs for typical in-plane resolutions of about 0.5 x 0.5 mm<sup>2</sup>. As a result, high-resolution positive contrast images of fibrous tissues can be generated within clinically feasible scan-time of about 2–7 minutes.</p></div></div>
<div class="section" id="abs1-4" xmlns="http://www.w3.org/1999/xhtml"><h4>Conclusion:</h4><div class="para"><p>After optimization, Fourier-encoded spoiled gradient echo provides a highly robust and flexible imaging technique for high-resolution positive contrast imaging of fibrous tissue that can readily be used in the clinical routine. Magn Reson Med, 2013. © 2012 Wiley Periodicals, Inc.</p></div></div>
]]></content:encoded><description>


Purpose:
The feasibility of imaging musculoskeletal fibrous tissue components, such as menisci, ligaments, and tendons, with a conventional spoiled gradient echo technique is explored in vivo at 3 T and 7 T.


Methods:
To this end, the echo time (TE1) of a conventional Fourier-encoded multicontrast three-dimensional SGPR sequence is minimized by using nonselective excitation pulses, highly asymmetric readouts, and a variable TE1 along the phase and slice encoding direction. In addition, a fully sampled second echo image (with TE2 &gt;&gt; TE1) can be used to highlight components with short transverse relaxation times in a difference image with positive contrast.


Results:
Fourier-encoded spoiled gradient echo sequences are able to provide sub-millisecond TE1 of about 800 μs for typical in-plane resolutions of about 0.5 x 0.5 mm2. As a result, high-resolution positive contrast images of fibrous tissues can be generated within clinically feasible scan-time of about 2–7 minutes.


Conclusion:
After optimization, Fourier-encoded spoiled gradient echo provides a highly robust and flexible imaging technique for high-resolution positive contrast imaging of fibrous tissue that can readily be used in the clinical routine. Magn Reson Med, 2013. © 2012 Wiley Periodicals, Inc.

</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fmrm.24580" xmlns="http://purl.org/rss/1.0/"><title>Contrast enhanced lung MRI in mice using 