Relativistic derivation of coupled spin-orbital angular momentum dynamics in magnetic systems, with total J conserved under Heisenberg exchange even in the presence of electromagnetic fields.
(2), specifically in the terms Hxc =−µ B σ·B xc eff + iµB 4m2c2 (p×B xc)·(p−eA)
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Relativistic theory for coupled orbital and spin angular momentum dynamics in magnetic systems
Relativistic derivation of coupled spin-orbital angular momentum dynamics in magnetic systems, with total J conserved under Heisenberg exchange even in the presence of electromagnetic fields.