Gauge invariance of the spin-other-orbit contribution to the g-tensors of electron paramagnetic resonance -: art. no. 214101

被引:22
|
作者
Patchkovskii, S
Strong, RT
Pickard, CJ
Un, S
机构
[1] Natl Res Council Canada, Steacie Inst Mol Sci, Ottawa, ON K1A 0R6, Canada
[2] Univ Cambridge, Cavendish Lab, Theory Condensed Matter Grp, Cambridge CB3 0HE, England
[3] CEA Saclay, Dept Biol Joliot Curie, Serv Bioenerget, CNRS,URA 2096, F-91191 Gif Sur Yvette, France
来源
JOURNAL OF CHEMICAL PHYSICS | 2005年 / 122卷 / 21期
基金
英国工程与自然科学研究理事会;
关键词
D O I
10.1063/1.1917840
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The spin-other-orbit (SOO) contribution to the g-tensor (Delta g(SOO)) of electron paramagnetic resonance arises due to the interaction of electron-spin magnetic moment with the magnetic field produced by the orbital motion of other electrons. A similar mechanism is responsible for the leading term in nuclear magnetic-shielding tensors sigma. We demonstrate that analogous to sigma, paramagnetic Delta g(SOO) contribution exhibits a pronounced dependence on the choice of the magnetic-field gauge. The gauge corrections to Delta g(SOO) are similar in magnitude, and opposite in sign, to the paramagnetic SOO term. We calculate gauge-invariant Delta g(SOO) values using gauge-including atomic orbitals and density-functional theory. For organic radicals, complete gauge-invariant Delta g(SOO) values typically amount to less than 500 parts per million (ppm), and are small compared to other g-tensor contributions. For the first-row transition-metal compounds, Delta g(SOO) may contribute several thousand ppm to the g-tensor, but are negligible compared to the remaining deviations from experiment. With popular choices for the magnetic-field gauge, the individual gauge-variant contributions may be an order of magnitude higher, and do not provide a reliable estimation of Delta g(SOO).
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页数:9
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