Magnetic anisotropy in density-functional theory

H. J. F. Jansen
Phys. Rev. B 38, 8022 – Published 15 October 1988
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Abstract

Magnetic anisotropy is discussed in terms of relativistic density-functional theory. Spin-orbit coupling in the kinetic energy operator of the Dirac equation is responsible for a nonzero value of the orbital angular momentum in cubic systems. Additional spin-orbit coupling terms originate from the Breit interaction between the electrons. The Hartree approximation to the Breit energy yields a magnetic dipole-dipole interaction, which is the cause of the magnetic shape anisotropy. All these terms have to be included in a discussion of the magnetic anisotropy of cubic systems.

  • Received 18 April 1988

DOI:https://doi.org/10.1103/PhysRevB.38.8022

©1988 American Physical Society

Authors & Affiliations

H. J. F. Jansen

  • Department of Physics, Oregon State University, Corvallis, Oregon 97331

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Issue

Vol. 38, Iss. 12 — 15 October 1988

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