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<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#"><channel rdf:about="http://onlinelibrary.wiley.com/rss/journal/10.1002/(ISSN)1552-504X" xmlns="http://purl.org/rss/1.0/"><title>Concepts in Magnetic Resonance Part B: Magnetic Resonance Engineering</title><description> Wiley Online Library : Concepts in Magnetic Resonance Part B: Magnetic Resonance Engineering</description><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2F%28ISSN%291552-504X</link><dc:publisher xmlns:dc="http://purl.org/dc/elements/1.1/">John Wiley &amp; Sons, Inc</dc:publisher><dc:language xmlns:dc="http://purl.org/dc/elements/1.1/">en</dc:language><dc:rights xmlns:dc="http://purl.org/dc/elements/1.1/">© 2013 Wiley Periodicals Inc.</dc:rights><prism:issn xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1552-5031</prism:issn><prism:eIssn xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1552-504X</prism:eIssn><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-01T00:00:00-05:00</dc:date><prism:coverDisplayDate xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">April 2013</prism:coverDisplayDate><prism:volume xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">43</prism:volume><prism:number xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">2</prism:number><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">I</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">II</prism:endingPage><image rdf:resource="http://onlinelibrary.wiley.com/store/10.1002/cmr.b.v43.2/asset/cover.gif?v=1&amp;s=7b8204dfbd5ad6c88586e7bcb63d7edbf4bdf58e"/><items><rdf:Seq><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21238"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21233"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21234"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21235"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21237"/></rdf:Seq></items></channel><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21238" xmlns="http://purl.org/rss/1.0/"><title>Editorial Board</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21238</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Editorial Board</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-24T21:35:40.048838-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cmr.b.21238</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/cmr.b.21238</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21238</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Editorial Board</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">i</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">i</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[]]></content:encoded><description/></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21233" xmlns="http://purl.org/rss/1.0/"><title>An advanced, integrated large-volume high-pressure autoclave and 1h/13c double-tuned resonator for chemistry and materials nuclear magnetic resonance spectroscopy and microscopy investigations</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21233</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">An advanced, integrated large-volume high-pressure autoclave and 1h/13c double-tuned resonator for chemistry and materials nuclear magnetic resonance spectroscopy and microscopy investigations</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Volker C. Behr, Martin W. Schmid, Robert A. Franich, Roger Meder</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-24T21:35:40.048838-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cmr.b.21233</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/cmr.b.21233</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21233</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Research Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">49</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">58</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>Nuclear magnetic resonance spectroscopy and imaging are well-established tools in chemistry, physics, and life sciences. Nevertheless, most applications are performed at room temperature and atmospheric pressure. To study the processes in supercritical fluids, sample containers and coils have to be redesigned to especially allow for higher pressures up to several hundred times the atmospheric pressure. In this study, we present a setup for performing spectroscopic and imaging experiments on wood immersed in supercritical CO<sub>2</sub> at up to 20 MPa for drying. A magnetic resonance-compatible autoclave as well as a double-tuned <sup>1</sup>H/<sup>13</sup>C-birdcage coil was designed and a setup for regulating pressure and storing gases was assembled. We were able to successfully perform measurements on the wood and water during the drying process and gaininsights into the displacement of water and its chemical reactions with the highly pressurized CO<sub>2</sub>. © 2013 Wiley Periodicals, Inc. Concepts Magn Reson Part B (Magn Reson Engineering) 43B: 49–58, 2013</p></div>
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Nuclear magnetic resonance spectroscopy and imaging are well-established tools in chemistry, physics, and life sciences. Nevertheless, most applications are performed at room temperature and atmospheric pressure. To study the processes in supercritical fluids, sample containers and coils have to be redesigned to especially allow for higher pressures up to several hundred times the atmospheric pressure. In this study, we present a setup for performing spectroscopic and imaging experiments on wood immersed in supercritical CO2 at up to 20 MPa for drying. A magnetic resonance-compatible autoclave as well as a double-tuned 1H/13C-birdcage coil was designed and a setup for regulating pressure and storing gases was assembled. We were able to successfully perform measurements on the wood and water during the drying process and gaininsights into the displacement of water and its chemical reactions with the highly pressurized CO2. © 2013 Wiley Periodicals, Inc. Concepts Magn Reson Part B (Magn Reson Engineering) 43B: 49–58, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21234" xmlns="http://purl.org/rss/1.0/"><title>A vertical-loop-array transmit coil for two-channel B1 shimming at 3T</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21234</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A vertical-loop-array transmit coil for two-channel B1 shimming at 3T</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Lae Hoon Kang, Yong Moon Park, Dong Eun Kim, Soo Yeol Lee</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-24T21:35:40.048838-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cmr.b.21234</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/cmr.b.21234</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21234</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Research Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">59</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">68</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>We propose a whole-body transmit coil structure for two-channel B<sub>1</sub> shimming at 3T. The transmit coil consists of four identical vertical-loop-coils placed on a cylindrical former by equiangular basis. A vertical loop coil consists of an inner-conductor plane and an outer-conductor plane both of which constitute a vertical loop when the two planes are connected by tuning capacitors at both ends. To improve the B<sub>1</sub> homogeneity of the transmit coil, we split the inner- and outer-conductor planes into two rungs. We made the transmit coil with the length of 500 mm on a frame that had the inner and outer diameters of 550mm and 600mm, respectively. In the B<sub>1</sub> shimming experiment with the transmit coil, we drove the coil with two RF power amplifiers of 18kWp each through two quadrature hybrids. Before the B<sub>1</sub> shimming, we performed B<sub>1</sub> mapping for each driving channel, and then, we determined the optimal magnitude and phase of the input signals to the RF power amplifiers. In the B<sub>1</sub> shimming experiment on a human-body-mimicking phantom, the optimized transmission improved the image uniformity by 24.7% as compared to the conventional quadrature transmission. © 2013 Wiley Periodicals, Inc. Concepts Magn Reson Part B (Magn Reson Engineering) 43B: 59–68, 2013</p></div>
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We propose a whole-body transmit coil structure for two-channel B1 shimming at 3T. The transmit coil consists of four identical vertical-loop-coils placed on a cylindrical former by equiangular basis. A vertical loop coil consists of an inner-conductor plane and an outer-conductor plane both of which constitute a vertical loop when the two planes are connected by tuning capacitors at both ends. To improve the B1 homogeneity of the transmit coil, we split the inner- and outer-conductor planes into two rungs. We made the transmit coil with the length of 500 mm on a frame that had the inner and outer diameters of 550mm and 600mm, respectively. In the B1 shimming experiment with the transmit coil, we drove the coil with two RF power amplifiers of 18kWp each through two quadrature hybrids. Before the B1 shimming, we performed B1 mapping for each driving channel, and then, we determined the optimal magnitude and phase of the input signals to the RF power amplifiers. In the B1 shimming experiment on a human-body-mimicking phantom, the optimized transmission improved the image uniformity by 24.7% as compared to the conventional quadrature transmission. © 2013 Wiley Periodicals, Inc. Concepts Magn Reson Part B (Magn Reson Engineering) 43B: 59–68, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21235" xmlns="http://purl.org/rss/1.0/"><title>Design of a quadrature surface coil for hyperpolarized 13C MRS cardiac metabolism studies in pigs</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21235</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Design of a quadrature surface coil for hyperpolarized 13C MRS cardiac metabolism studies in pigs</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">G. Giovannetti, F. Frijia, V. Hartwig, S. Attanasio, L. Menichetti, N. Vanello, V. Positano, J.H. Ardenkjaer-Larsen, V. Lionetti, G.D. Aquaro, D. De Marchi, R.F. Schulte, F. Wiesinger, L. Landini, M. Lombardi, M.F. Santarelli</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-24T21:35:40.048838-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cmr.b.21235</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/cmr.b.21235</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21235</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Research Article</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">69</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">77</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>This work describes the design of a quadrature surface coil constituted by a circular loop and a butterfly coil, employed in transmit/receive (TX/RX) mode for hyperpolarized <sup>13</sup>C studies of pig heart with a clinical 3T scanner. The coil characterization is performed by developing an SNR model for coil performance evaluation in terms of coil resistance, sample-induced resistance and magnetic field pattern. Experimental SNR-vs.-depth profiles, extracted from the [1–13C]acetate phantom chemical shift image (CSI), showed good agreement with the theoretical SNR-vs.-depth profiles. Moreover, the performance of the quadrature coil was compared with the single TX/RX circular and TX/RX butterfly coil, in order to verify the advantage of the proposed configuration over the single coils throughout the volume of interest for cardiac imaging in pig. Finally, the quadrature surface coil was tested by acquiring metabolic maps with hyperpolarized [1–13C]pyruvate injected i.v. in a pig. © 2013 Wiley Periodicals, Inc. Concepts Magn Reson Part B (Magn Reson Engineering) 43B: 69–77, 2013</p></div>
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This work describes the design of a quadrature surface coil constituted by a circular loop and a butterfly coil, employed in transmit/receive (TX/RX) mode for hyperpolarized 13C studies of pig heart with a clinical 3T scanner. The coil characterization is performed by developing an SNR model for coil performance evaluation in terms of coil resistance, sample-induced resistance and magnetic field pattern. Experimental SNR-vs.-depth profiles, extracted from the [1–13C]acetate phantom chemical shift image (CSI), showed good agreement with the theoretical SNR-vs.-depth profiles. Moreover, the performance of the quadrature coil was compared with the single TX/RX circular and TX/RX butterfly coil, in order to verify the advantage of the proposed configuration over the single coils throughout the volume of interest for cardiac imaging in pig. Finally, the quadrature surface coil was tested by acquiring metabolic maps with hyperpolarized [1–13C]pyruvate injected i.v. in a pig. © 2013 Wiley Periodicals, Inc. Concepts Magn Reson Part B (Magn Reson Engineering) 43B: 69–77, 2013
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21237" xmlns="http://purl.org/rss/1.0/"><title>NMR Concepts</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21237</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">NMR Concepts</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-24T21:35:40.048838-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/cmr.b.21237</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/cmr.b.21237</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fcmr.b.21237</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">NMR Concepts</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">I</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">II</prism:endingPage><content:encoded xmlns:content="http://purl.org/rss/1.0/modules/content/"><![CDATA[]]></content:encoded><description/></item></rdf:RDF>