The first application of current density functional theory (CDFT) to spontaneously magnetised solids is presented. We show that non-relativistic CDFT without spin-orbit coupling does not lead to finite orbital currents. In accordance with experiment, an enhancement of the spin-orbit–induced orbital magnetic moment is found for the ferromagnets Fe and Co, while for Ni only a minor change was found compared to a plain calculation done within spin density functional theory (SDFT).
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Ebert et al. (1997) studied this question.
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