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Spin-orbit coupling in Fe-based superconductors of the spin-rotational invariance in the spin-liquid phase can occur due to spin-orbit coupling. We study

Spin-orbit coupling in Fe-based superconductors of the spin-rotational invariance in the spin-liquid phase can occur due to spin-orbit coupling. We study

Spin-orbit coupling of sp2 nanocarbons and magnetism of fullerene C60 in view of spin peculiarities of unrestricted Hartree–Fock solution to the consideration of spin-orbit coupling (SOC) of open-shell systems in general and sp2 nanocarbons in particular

Spin-orbit coupling of sp2 nanocarbons and magnetism of fullerene C60 in view of spin peculiarities of unrestricted Hartree-Fock solutionSpin-orbit coupling of sp2 nanocarbons and magnetism of fullerene C60 in view of spin peculiarities

Spin relaxation times of donor centers associated with lithium in monoisotopic 28Si-Orbach process, with the parameters of the spin-orbit coupling ~ 1·10-6 meV compare to Orbach process for Li

Localization the pump-induced electron interaction and of spin-orbital coupling or the near-lying singlet and triplet excited states in the impurity generation of light in the series multiatomic moleculesLocalization the pump-induced electron interaction and of spin-orbital coupling or the near-lying

Spin-orbit coupling from a two-component self-consistent approach. II. Non-collinear density functional theoriesSpin-orbit coupling from a two-component self-consistent approach. II. Non-collinear density

Spin-orbit coupling in periodic systems with broken time-reversal symmetry: Formal and computational aspectsSpin-orbit coupling in periodic systems with broken time-reversal symmetry: Formal

Spin relaxation times of donor centers associated with lithium in monoisotopic 28Si-Orbach process, with the parameters of the spin-orbit coupling ~ 1·10-6 meV compare to Orbach process for Li

Electronic theory for the magnetic anisotropy in Sr2RuO 4 that because of spin-orbit coupling the out-of-plane component of the spin susceptibility χzz(q, ω) becomes two

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