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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)1521-3889" xmlns="http://purl.org/rss/1.0/"><title>Annalen der Physik</title><description> Wiley Online Library : Annalen der Physik</description><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2F%28ISSN%291521-3889</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/">Copyright © 2013 WILEY-VCH Verlag GmbH &amp; Co. KGaA, Weinheim</dc:rights><prism:issn xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">0003-3804</prism:issn><prism:eIssn xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">1521-3889</prism:eIssn><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-01T00:00:00-05:00</dc:date><prism:coverDisplayDate xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">May 2013</prism:coverDisplayDate><prism:volume xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">525</prism:volume><prism:number xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">5</prism:number><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">323</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">394</prism:endingPage><image rdf:resource="http://onlinelibrary.wiley.com/store/10.1002/andp.v525.5/asset/cover.gif?v=1&amp;s=113f085cfb8b43912c7263dcb61f455776638622"/><items><rdf:Seq><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300062"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300036"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300013"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300039"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300010"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200261"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370050"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370051"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370052"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370053"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370054"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370055"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300725"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300724"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370056"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200227"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200272"/><rdf:li rdf:resource="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200271"/></rdf:Seq></items></channel><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300062" xmlns="http://purl.org/rss/1.0/"><title>Frequency-comb spectroscopy of the hydrogen 1S-3S and 1S-3D transitions</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300062</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Frequency-comb spectroscopy of the hydrogen 1S-3S and 1S-3D transitions</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Elisabeth Peters, Dylan C. Yost, Arthur Matveev, Theodor W. Hänsch, Thomas Udem</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-17T03:22:29.956001-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201300062</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/andp.201300062</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300062</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Rapid Research Letter</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>An observation of the 1S-3S and 1S-3D two-photon transitions in an atomic hydrogen beam using direct frequency-comb spectroscopy in a Doppler-free arrangement is reported. The measurements of these transition frequencies may be used for an improved determination of the Rydberg constant and the 1S Lamb shift and could shed light on the current discrepancy in the determination of the proton charge radius. Concurrently, a frequency comb well-suited for high-precision, Doppler-free spectroscopy in the deep ultraviolet (DUV) wavelength region is demonstrated.</p></div>]]></content:encoded><description>

An observation of the 1S-3S and 1S-3D two-photon transitions in an atomic hydrogen beam using direct frequency-comb spectroscopy in a Doppler-free arrangement is reported. The measurements of these transition frequencies may be used for an improved determination of the Rydberg constant and the 1S Lamb shift and could shed light on the current discrepancy in the determination of the proton charge radius. Concurrently, a frequency comb well-suited for high-precision, Doppler-free spectroscopy in the deep ultraviolet (DUV) wavelength region is demonstrated.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300036" xmlns="http://purl.org/rss/1.0/"><title>A dual-isotope rubidium comagnetometer to search for anomalous long-range spin-mass (spin-gravity) couplings of the proton</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300036</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">A dual-isotope rubidium comagnetometer to search for anomalous long-range spin-mass (spin-gravity) couplings of the proton</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Derek F. Jackson Kimball, Ian Lacey, Julian Valdez, Jerlyn Swiatlowski, Cesar Rios, Rodrigo Peregrina-Ramirez, Caitlin Montcrieffe, Jackie Kremer, Jordan Dudley, C. Sanchez</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-16T05:23:21.186548-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201300036</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/andp.201300036</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300036</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original 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 experimental concept of a search for a long-range coupling between rubidium (Rb) nuclear spins and the mass of the Earth is described. The experiment is based on simultaneous measurement of the spin precession frequencies for overlapping ensembles of <sup>85</sup>Rb and <sup>87</sup>Rb atoms contained within an evacuated, antirelaxation-coated vapor cell. Rubidium atoms are spin-polarized in the presence of an applied magnetic field by synchronous optical pumping with circularly polarized laser light. Spin precession is probed by measuring optical rotation of far-off-resonant, linearly polarized laser light. Simultaneous measurement of <sup>85</sup>Rb and <sup>87</sup>Rb spin precession frequencies enables suppression of magnetic-field-related systematic effects. The nuclear structure of the Rb isotopes makes the experiment particularly sensitive to anomalous spin-dependent interactions of the proton. Experimental sensitivity and a variety of systematic effects are discussed, and initial data are presented.</p></div>]]></content:encoded><description>

The experimental concept of a search for a long-range coupling between rubidium (Rb) nuclear spins and the mass of the Earth is described. The experiment is based on simultaneous measurement of the spin precession frequencies for overlapping ensembles of 85Rb and 87Rb atoms contained within an evacuated, antirelaxation-coated vapor cell. Rubidium atoms are spin-polarized in the presence of an applied magnetic field by synchronous optical pumping with circularly polarized laser light. Spin precession is probed by measuring optical rotation of far-off-resonant, linearly polarized laser light. Simultaneous measurement of 85Rb and 87Rb spin precession frequencies enables suppression of magnetic-field-related systematic effects. The nuclear structure of the Rb isotopes makes the experiment particularly sensitive to anomalous spin-dependent interactions of the proton. Experimental sensitivity and a variety of systematic effects are discussed, and initial data are presented.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300013" xmlns="http://purl.org/rss/1.0/"><title>Steady state ensembles of thermal radiation in a layered media with a constant heat flux</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300013</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Steady state ensembles of thermal radiation in a layered media with a constant heat flux</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Bair V. Budaev, David B. Bogy</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-10T11:27:34.484585-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201300013</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/andp.201300013</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300013</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original 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>This paper describes steady-state ensembles of thermally excited electromagnetic radiation in nano-scale layered media with a constant non-vanishing heat flux across the layers. It is shown that Planck's law of thermal radiation, the principle of equivalence, and the laws of wave propagation in layered media, imply that in order for the ensemble of thermally excited electromagnetic fields to exist in a medium consisting of a stack of layers between two half-space, the net heat flux across the layers must exceed a certain threshold that is determined by the temperatures of the half spaces and by the reflective properties of the entire structure. The obtained results provide a way for estimating the radiative heat transfer coefficient of nano-scale layered structures.</p></div>
]]></content:encoded><description>
This paper describes steady-state ensembles of thermally excited electromagnetic radiation in nano-scale layered media with a constant non-vanishing heat flux across the layers. It is shown that Planck's law of thermal radiation, the principle of equivalence, and the laws of wave propagation in layered media, imply that in order for the ensemble of thermally excited electromagnetic fields to exist in a medium consisting of a stack of layers between two half-space, the net heat flux across the layers must exceed a certain threshold that is determined by the temperatures of the half spaces and by the reflective properties of the entire structure. The obtained results provide a way for estimating the radiative heat transfer coefficient of nano-scale layered structures.
</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300039" xmlns="http://purl.org/rss/1.0/"><title>Mass measurements of singly and highly charged radioactive ions at TITAN: A new QEC-value measurement of 10C</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300039</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Mass measurements of singly and highly charged radioactive ions at TITAN: A new QEC-value measurement of 10C</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Anna A. Kwiatkowski, Ankur Chaudhuri, Usman Chowdhury, Aaron T. Gallant, Tegan D. Macdonald, Bradley E. Schultz, Martin C. Simon, Jens Dilling</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-30T05:12:32.673299-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201300039</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/andp.201300039</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300039</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original 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>Superallowed β-decay strengths or corrected <img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/andp.201300039/asset/equation/andp201300039-math-0001.png?v=1&amp;t=hgvp44lo&amp;s=27bcb486683a7bc3a97d30fe360dc7e49eb0cd6e" class="inlineGraphic"/> values provide some of the most stringent limits for physics beyond the standard three-quark model. For this reason, the <img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/andp.201300039/asset/equation/andp201300039-math-0002.png?v=1&amp;t=hgvp44lp&amp;s=d282dab9d52a0ca985953f584160f0fa7ec33040" class="inlineGraphic"/>-value <sup>10</sup>C has been measured and found to be 3468.31(51) keV with the TITAN Penning trap mass spectrometer. The facility is unique in coupling such an online spectrometer to a charge breeder, permitting a mass measurement of another superallowed β-emitter, <sup>74</sup>Rb, in the 8+ charge state. An overview of the TITAN facility and recent highlights are presented alongside the new <img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/andp.201300039/asset/equation/andp201300039-math-0003.png?v=1&amp;t=hgvp44lr&amp;s=8befb0d2645c519a687b26eaafe8eefa3145ed99" class="inlineGraphic"/>-value determination of <sup>10</sup>C.</p></div>]]></content:encoded><description>
Superallowed β-decay strengths or corrected Ft values provide some of the most stringent limits for physics beyond the standard three-quark model. For this reason, the QEC-value 10C has been measured and found to be 3468.31(51) keV with the TITAN Penning trap mass spectrometer. The facility is unique in coupling such an online spectrometer to a charge breeder, permitting a mass measurement of another superallowed β-emitter, 74Rb, in the 8+ charge state. An overview of the TITAN facility and recent highlights are presented alongside the new QEC-value determination of 10C.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300010" xmlns="http://purl.org/rss/1.0/"><title>Microwave and submillimeter molecular transitions and their dependence on fundamental constants</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300010</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Microwave and submillimeter molecular transitions and their dependence on fundamental constants</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Mikhail G. Kozlov, Sergei A. Levshakov</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T06:46:39.680565-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201300010</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/andp.201300010</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300010</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>Microwave and submillimeter molecular transition frequencies between nearly degenerated rotational levels, tunneling transitions, and mixed tunneling-rotational transitions show an extremely high sensitivity to the values of the fine-structure constant, α, and the electron-to-proton mass ratio, μ. This review summarizes the theoretical background on quantum-mechanical calculations of the sensitivity coefficients of such transitions to tiny changes in α and μ for a number of molecules which are usually observed in Galactic and extragalactic sources, and discusses the possibility of testing the space- and time-invariance of fundamental constants through comparison between precise laboratory measurements of the molecular rest frequencies and their astronomical counterparts. In particular, diatomic radicals CH, OH, NH<sup>+</sup>, and a linear polyatomic radical C<sub>3</sub>H in Π electronic ground state, polyatomic molecules NH<sub>3</sub>, ND<sub>3</sub>, NH<sub>2</sub>D, NHD<sub>2</sub>, H<sub>2</sub>O<sub>2</sub>, H<sub>3</sub>O<sup>+</sup>, CH<sub>3</sub>OH, and CH<sub>3</sub>NH<sub>2</sub> in their tunneling and tunneling-rotational modes are considered. It is shown that sensitivity coefficients strongly depend on the quantum numbers of the corresponding transitions. This can be used for astrophysical tests of Einstein's Equivalence Principle all over the Universe at an unprecedented level of sensitivity of <img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/andp.201300010/asset/equation/andp201300010-math-0001.png?v=1&amp;t=hgvp44ly&amp;s=a62143342a73b6757c89ddc93de8aa049faaa378" class="inlineGraphic"/>, which is a limit three to two orders of magnitude lower as compared to the current constraints on cosmological variations of α and μ: <img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/andp.201300010/asset/equation/andp201300010-math-0002.png?v=1&amp;t=hgvp44m0&amp;s=c6f99c3465a33c63710eb6d25f6f0e776693410b" class="inlineGraphic"/> <img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/andp.201300010/asset/equation/andp201300010-math-0003.png?v=1&amp;t=hgvp44m0&amp;s=2f6edb83a8f6599a0388d166fe31bc99d1dfa973" class="inlineGraphic"/>, <img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/andp.201300010/asset/equation/andp201300010-math-0004.png?v=1&amp;t=hgvp44m1&amp;s=526fd1dfaef2a64951b0e745cbeab0aa480ec1ca" class="inlineGraphic"/> <img alt="inline image" src="http://onlinelibrary.wiley.com/store/10.1002/andp.201300010/asset/equation/andp201300010-math-0005.png?v=1&amp;t=hgvp44m1&amp;s=8f2ac15bb23eb62953a3a72180b83c14c6352dda" class="inlineGraphic"/>.</p></div>]]></content:encoded><description>
Microwave and submillimeter molecular transition frequencies between nearly degenerated rotational levels, tunneling transitions, and mixed tunneling-rotational transitions show an extremely high sensitivity to the values of the fine-structure constant, α, and the electron-to-proton mass ratio, μ. This review summarizes the theoretical background on quantum-mechanical calculations of the sensitivity coefficients of such transitions to tiny changes in α and μ for a number of molecules which are usually observed in Galactic and extragalactic sources, and discusses the possibility of testing the space- and time-invariance of fundamental constants through comparison between precise laboratory measurements of the molecular rest frequencies and their astronomical counterparts. In particular, diatomic radicals CH, OH, NH+, and a linear polyatomic radical C3H in Π electronic ground state, polyatomic molecules NH3, ND3, NH2D, NHD2, H2O2, H3O+, CH3OH, and CH3NH2 in their tunneling and tunneling-rotational modes are considered. It is shown that sensitivity coefficients strongly depend on the quantum numbers of the corresponding transitions. This can be used for astrophysical tests of Einstein's Equivalence Principle all over the Universe at an unprecedented level of sensitivity of ∼10−9, which is a limit three to two orders of magnitude lower as compared to the current constraints on cosmological variations of α and μ: Δα/α &lt;10−6, Δμ/μ &lt;10−7.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200261" xmlns="http://purl.org/rss/1.0/"><title>Circuit QED lattices</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200261</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Circuit QED lattices</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Sebastian Schmidt, Jens Koch</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-26T06:40:48.232824-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201200261</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/andp.201200261</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200261</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[
<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 Jaynes-Cummings model describes the coupling between photons and a single two-level atom in a simplified representation of light-matter interactions. In circuit QED, this model is implemented by combining microwave resonators and superconducting qubits on a microchip with unprecedented experimental control. Arranging qubits and resonators in the form of a lattice realizes a new kind of Hubbard model, the Jaynes-Cummings-Hubbard model, in which the elementary excitations are polariton quasi-particles. Due to the genuine openness of photonic systems, circuit QED lattices offer the possibility to study the intricate interplay of collective behavior, strong correlations and non-equilibrium physics. Thus, turning circuit QED into an architecture for quantum simulation, i.e., using a well-controlled system to mimic the intricate quantum behavior of another system too daunting for a theorist to tackle head-on, is an exciting idea which has served as theorists’ playground for a while and is now also starting to catch on in experiments. This review gives a summary of the most recent theoretical proposals and experimental efforts.</p></div>]]></content:encoded><description>

The Jaynes-Cummings model describes the coupling between photons and a single two-level atom in a simplified representation of light-matter interactions. In circuit QED, this model is implemented by combining microwave resonators and superconducting qubits on a microchip with unprecedented experimental control. Arranging qubits and resonators in the form of a lattice realizes a new kind of Hubbard model, the Jaynes-Cummings-Hubbard model, in which the elementary excitations are polariton quasi-particles. Due to the genuine openness of photonic systems, circuit QED lattices offer the possibility to study the intricate interplay of collective behavior, strong correlations and non-equilibrium physics. Thus, turning circuit QED into an architecture for quantum simulation, i.e., using a well-controlled system to mimic the intricate quantum behavior of another system too daunting for a theorist to tackle head-on, is an exciting idea which has served as theorists’ playground for a while and is now also starting to catch on in experiments. This review gives a summary of the most recent theoretical proposals and experimental efforts.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370050" xmlns="http://purl.org/rss/1.0/"><title>Cover Picture: Ann. Phys. 5'2013</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370050</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Cover Picture: Ann. Phys. 5'2013</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-02T06:02:29.414167-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201370050</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/andp.201370050</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370050</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Cover Picture</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">NA</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">NA</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>General relativity may be formulated in terms of tetrad fields and of the torsion tensor, i.e. in an alternative geometrical formulation as shown in the review by J.W. Maluf (pp. 339–357). This teleparallel equivalent of general relativity has been expressed on the front page in an artistic vision by G. Schulz (Fussgoenheim, Germany).</p></div><a title="Link to full-size graphical abstract" class="figZoom" href="http://onlinelibrary.wiley.com/store/10.1002/andp.201370050/asset/image_m/andp201370050-gra-0001-m.jpg?v=1&amp;s=62b7da54d4d7155c984e452e7f0e15ad12670adf" xmlns="http://www.w3.org/1999/xhtml"><img alt="Thumbnail image of graphical abstract" title="Thumbnail image of graphical abstract" src="http://onlinelibrary.wiley.com/store/10.1002/andp.201370050/asset/image_n/andp201370050-gra-0001.gif?v=1&amp;s=39b38dca334deea1567b52199723492185c07a2c"/></a>
<div class="para" xmlns="http://www.w3.org/1999/xhtml"><p>General relativity may be formulated in terms of tetrad fields and of the torsion tensor, i.e. in an alternative geometrical formulation as shown in the review by J.W. Maluf (pp. 339–357). This teleparallel equivalent of general relativity has been expressed on the front page in an artistic vision by G. Schulz (Fussgoenheim, Germany).
</p><!--Unmatched element: w:blockFixed--></div>
]]></content:encoded><description>
General relativity may be formulated in terms of tetrad fields and of the torsion tensor, i.e. in an alternative geometrical formulation as shown in the review by J.W. Maluf (pp. 339–357). This teleparallel equivalent of general relativity has been expressed on the front page in an artistic vision by G. Schulz (Fussgoenheim, Germany).General relativity may be formulated in terms of tetrad fields and of the torsion tensor, i.e. in an alternative geometrical formulation as shown in the review by J.W. Maluf (pp. 339–357). This teleparallel equivalent of general relativity has been expressed on the front page in an artistic vision by G. Schulz (Fussgoenheim, Germany).






</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370051" xmlns="http://purl.org/rss/1.0/"><title>Issue Information: Ann. Phys. 5'2013</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370051</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Issue Information: Ann. Phys. 5'2013</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-02T06:02:29.414167-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201370051</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/andp.201370051</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370051</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Issue Information</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">NA</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">NA</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%2Fandp.201370052" xmlns="http://purl.org/rss/1.0/"><title>Call For Papers: Ann. Phys. 5'2013</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370052</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Call For Papers: Ann. Phys. 5'2013</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-02T06:02:29.414167-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201370052</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/andp.201370052</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370052</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Call for Papers</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A57</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A57</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%2Fandp.201370053" xmlns="http://purl.org/rss/1.0/"><title>Contents: Ann. Phys. 5'2013</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370053</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Contents: Ann. Phys. 5'2013</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-02T06:02:29.414167-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201370053</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/andp.201370053</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370053</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Contents</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A58</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A59</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%2Fandp.201370054" xmlns="http://purl.org/rss/1.0/"><title>Advisory Board</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370054</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Advisory 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/">2013-05-02T06:02:29.414167-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201370054</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/andp.201370054</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370054</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Advisory Board</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A60</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A60</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%2Fandp.201370055" xmlns="http://purl.org/rss/1.0/"><title>RETROSPECT – Highlights from recent Annalen der Physik issues</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370055</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">RETROSPECT – Highlights from recent Annalen der Physik issues</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-02T06:02:29.414167-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201370055</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/andp.201370055</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370055</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Retrospect</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A61</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A61</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%2Fandp.201300725" xmlns="http://purl.org/rss/1.0/"><title>The discovery of the Stark effect and its early theoretical explanations</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300725</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The discovery of the Stark effect and its early theoretical explanations</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">A. J. Kox</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-02T06:02:29.414167-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201300725</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/andp.201300725</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300725</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">THEN &amp; NOW</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A63</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A66</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%2Fandp.201300724" xmlns="http://purl.org/rss/1.0/"><title>Darkness: What comprises empty space?</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300724</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Darkness: What comprises empty space?</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">James Bjorken</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-02T06:02:29.414167-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201300724</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/andp.201300724</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201300724</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">PERSPECTIVES &amp; VIEWS</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A67</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A79</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%2Fandp.201370056" xmlns="http://purl.org/rss/1.0/"><title>Special Features</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370056</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Special Features</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/"/><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-05-02T06:02:29.414167-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201370056</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/andp.201370056</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201370056</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Special Features</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A80</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">A80</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%2Fandp.201200227" xmlns="http://purl.org/rss/1.0/"><title>Observational effects from quantum cosmology</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200227</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Observational effects from quantum cosmology</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Gianluca Calcagni</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-12T02:54:57.653317-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201200227</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/andp.201200227</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200227</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/">323</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">338</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 status of quantum cosmologies as testable models of the early universe is assessed in the context of inflation. While traditional Wheeler–DeWitt quantization is unable to produce sizable effects in the cosmic microwave background, the more recent loop quantum cosmology can generate potentially detectable departures from the standard cosmic spectrum. Thus, present observations constrain the parameter space of the model, which could be made falsifiable by near-future experiments.</p></div>]]></content:encoded><description>
The status of quantum cosmologies as testable models of the early universe is assessed in the context of inflation. While traditional Wheeler–DeWitt quantization is unable to produce sizable effects in the cosmic microwave background, the more recent loop quantum cosmology can generate potentially detectable departures from the standard cosmic spectrum. Thus, present observations constrain the parameter space of the model, which could be made falsifiable by near-future experiments.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200272" xmlns="http://purl.org/rss/1.0/"><title>The teleparallel equivalent of general relativity</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200272</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">The teleparallel equivalent of general relativity</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">José W. Maluf</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-03-15T08:03:56.107459-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201200272</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/andp.201200272</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200272</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/">339</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">357</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>A review of the teleparallel equivalent of general relativity is presented. It is emphasized that general relativity may be formulated in terms of the tetrad fields and of the torsion tensor, and that this geometrical formulation leads to alternative insights into the theory. The equivalence with the standard formulation in terms of the metric and curvature tensors takes place at the level of field equations. The review starts with a brief account of the history of teleparallel theories of gravity. Then the ordinary interpretation of the tetrad fields as reference frames adapted to arbitrary observers in space–time is discussed, and the tensor of inertial accelerations on frames is obtained. It is shown that the Lagrangian and Hamiltonian field equations allow us to define the energy, momentum and angular momentum of the gravitational field, as surface integrals of the field quantities. In the phase space of the theory, these quantities satisfy the algebra of the Poincaré group.</p></div>]]></content:encoded><description>
A review of the teleparallel equivalent of general relativity is presented. It is emphasized that general relativity may be formulated in terms of the tetrad fields and of the torsion tensor, and that this geometrical formulation leads to alternative insights into the theory. The equivalence with the standard formulation in terms of the metric and curvature tensors takes place at the level of field equations. The review starts with a brief account of the history of teleparallel theories of gravity. Then the ordinary interpretation of the tetrad fields as reference frames adapted to arbitrary observers in space–time is discussed, and the tensor of inertial accelerations on frames is obtained. It is shown that the Lagrangian and Hamiltonian field equations allow us to define the energy, momentum and angular momentum of the gravitational field, as surface integrals of the field quantities. In the phase space of the theory, these quantities satisfy the algebra of the Poincaré group.</description></item><item rdf:about="http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200271" xmlns="http://purl.org/rss/1.0/"><title>Next-to-next-to-leading order post-Newtonian linear-in-spin binary Hamiltonians</title><link>http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200271</link><dc:title xmlns:dc="http://purl.org/dc/elements/1.1/">Next-to-next-to-leading order post-Newtonian linear-in-spin binary Hamiltonians</dc:title><dc:creator xmlns:dc="http://purl.org/dc/elements/1.1/">Johannes Hartung, Jan Steinhoff, Gerhard Schäfer</dc:creator><dc:date xmlns:dc="http://purl.org/dc/elements/1.1/">2013-04-24T01:06:48.847239-05:00</dc:date><dc:identifier xmlns:dc="http://purl.org/dc/elements/1.1/">doi:10.1002/andp.201200271</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/andp.201200271</prism:doi><prism:url xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">http://onlinelibrary.wiley.com/resolve/doi?DOI=10.1002%2Fandp.201200271</prism:url><prism:section xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">Original Paper</prism:section><prism:startingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">359</prism:startingPage><prism:endingPage xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/">394</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 next-to-next-to-leading order post-Newtonian spin-orbit and spin(1)-spin(2) Hamiltonians for binary compact objects in general relativity are derived. The Arnowitt-Deser-Misner canonical formalism and its generalization to spinning compact objects in general relativity are presented and a fully reduced matter-only Hamiltonian is obtained. Several simplifications using integrations by parts are discussed. Approximate solutions to the constraints and evolution equations of motion are provided. Technical details of the integration procedures are given including an analysis of the short-range behavior of the integrands around the sources. The Hamiltonian of a test-spin moving in a stationary Kerr spacetime is obtained by rather simple approach and used to check parts of the mentioned results. Kinematical consistency checks by using the global (post-Newtonian approximate) Poincaré algebra are applied. Along the way a self-contained overview for the computation of the 3PN ADM point-mass Hamiltonian is provided, too.</p></div>]]></content:encoded><description>
The next-to-next-to-leading order post-Newtonian spin-orbit and spin(1)-spin(2) Hamiltonians for binary compact objects in general relativity are derived. The Arnowitt-Deser-Misner canonical formalism and its generalization to spinning compact objects in general relativity are presented and a fully reduced matter-only Hamiltonian is obtained. Several simplifications using integrations by parts are discussed. Approximate solutions to the constraints and evolution equations of motion are provided. Technical details of the integration procedures are given including an analysis of the short-range behavior of the integrands around the sources. The Hamiltonian of a test-spin moving in a stationary Kerr spacetime is obtained by rather simple approach and used to check parts of the mentioned results. Kinematical consistency checks by using the global (post-Newtonian approximate) Poincaré algebra are applied. Along the way a self-contained overview for the computation of the 3PN ADM point-mass Hamiltonian is provided, too.</description></item></rdf:RDF>