2018
DOI: 10.1016/j.physb.2017.08.063
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Mean-field study of correlation-induced antisymmetric spin-orbit coupling in a two-orbital honeycomb model

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Cited by 4 publications
(6 citation statements)
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“…The axial 2nd-rank magneto-electric (current) tensor α is obtained by using Âi = Mi and Bj = Ĵj in Eq. (43). As Mi is time-reversal odd and spatial inversion even, the dissipative part α(J) becomes nonzero in the absence of only the spatial inversion symmetry.…”
Section: Magneto-electric(current) Tensormentioning
confidence: 98%
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“…The axial 2nd-rank magneto-electric (current) tensor α is obtained by using Âi = Mi and Bj = Ĵj in Eq. (43). As Mi is time-reversal odd and spatial inversion even, the dissipative part α(J) becomes nonzero in the absence of only the spatial inversion symmetry.…”
Section: Magneto-electric(current) Tensormentioning
confidence: 98%
“…namely, we adopt Âi = Bi = Ĵi in the general formula (43). As the electric current operator Ĵi is both timereversal and spatial-inversion odd, the polar electric conductivity tensor σ(E) (electric-field driven non-dissipative part) becomes nonzero only when the time-reversal symmetry is broken, while there is no symmetry restriction for the current driven dissipative part σ(J) .…”
Section: Electric Conductivity Tensormentioning
confidence: 99%
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“…The staggered electronic orders are accompanied by the oddparity multipoles, such as magnetic quadrupole 27 , electric octupole 28 , and magnetic toroidal dipoles 10,11,22,[29][30][31][32][33][34] . A mi-croscopic theory has recently been elucidated by the authors through the systematic analysis of staggered charge, spin, and orbital orderings in a minimal model on a honeycomb structure 26,31,35 . The authors constructed a classification of the staggered orderings and associated odd-parity multipoles, and clarified how the ASOC is induced in each case.…”
Section: Introductionmentioning
confidence: 99%