2014
DOI: 10.1002/cphc.201402121
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Nuclear‐Spin‐Induced Cotton–Mouton Effect in a Strong External Magnetic Field

Abstract: Novel, high-sensitivity and high-resolution spectroscopic methods can provide site-specific nuclear information by exploiting nuclear magneto-optic properties. We present a first-principles electronic structure formulation of the recently proposed nuclear-spin-induced Cotton-Mouton effect in a strong external magnetic field (NSCM-B). In NSCM-B, ellipticity is induced in a linearly polarized light beam, which can be attributed to both the dependence of the symmetric dynamic polarizability on the external magnet… Show more

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Cited by 14 publications
(22 citation statements)
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“…The differences in rotation between molecules have already been experimentally verified5, while high-resolution nuclear site specificity still awaits experimental confirmation. While NSOR is the only experimentally observed NMOS effect to date, its discovery has inspired a number of theoretical works suggesting existence of further effects691213141516, among them the NSCD, the focus of this paper.…”
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confidence: 99%
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“…The differences in rotation between molecules have already been experimentally verified5, while high-resolution nuclear site specificity still awaits experimental confirmation. While NSOR is the only experimentally observed NMOS effect to date, its discovery has inspired a number of theoretical works suggesting existence of further effects691213141516, among them the NSCD, the focus of this paper.…”
mentioning
confidence: 99%
“…Recent years have seen both experimental progress12345 in, as well as many theoretical proposals678910111213141516 of, spectroscopies based on nuclear magneto-optic phenomena (termed nuclear magneto-optic spectroscopy, NMOS). NMOS methods, which manifest themselves through modulation of the polarization state of light passing through a nuclear spin-polarized sample, can be thought of as analogues of the classical magneto-optic phenomena17, formally obtained by exchanging the externally applied magnetic field by the field originating from a macroscopic magnetization of an ensemble of nuclear spins.…”
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confidence: 99%
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“…3, 5. Then the magnetic linear birefringence (the Cotton–Mouton effect) is induced by the external magnetic field B 0 , prepolarized nuclear magnetic moment ${m_z^{({\rm{I}})} }$ , and their cross effect ${B_0 m_z^{({\rm{I}})} }$ ,1013 which makes linearly polarized incident light become elliptically polarized light with ellipticity angle ψ C–M through the medium. How do we distinguish IR‐NSCD ( ψ IR ) from the Cotton–Mouton effect ψ C–M in the experiment?…”
Section: Discussionmentioning
confidence: 99%
“…[3,5]. Then the magnetic linear birefringence (the Cotton-Mouton effect) is induced by the external magnetic field B 0 ,p repolarized nuclear magnetic moment m ðIÞ z ,a nd their cross effect B 0 m ðIÞ z , [10][11][12][13] which makes linearly polarized incident light become elliptically polarized light with ellipticity angle y C-M through the medium. How do we distinguish IR-NSCD (y IR ) from the Cotton-Mouton effect y C-M in the experiment?A si n Refs.…”
Section: Distinguishing Ir-nscd From the Cotton-mouton Effectmentioning
confidence: 99%