4.6 Article

Implementation of the relativistic effects on spin in first-principles electronic structure and magnetic property calculations

期刊

CHINESE JOURNAL OF PHYSICS
卷 77, 期 -, 页码 1579-1586

出版社

ELSEVIER
DOI: 10.1016/j.cjph.2021.12.019

关键词

Extended Hamiltonian; Spin-orbit coupling; Magnetic moment; Spin-orbit torque; Landau-Lifshitz damping; 3d transition metals

资金

  1. Ministry of Science and Technology, Taiwan [MOST 108-2628-M-008-004-MY3]
  2. National Center for Theoretical Sciences, Taiwan

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This study applied an extended single Hamiltonian to investigate relativistic effects in atoms, including spin-orbit coupling and coupling with electric fields. The results show that spin-orbit coupling affects the behavior of electrons in metals and explain the Lorentzian broadening phenomenon at low temperatures.
An extended single Hamiltonian, which can properly treat the couplings between the two spin states, has been applied to study the relativistic effects including the spin-orbit coupling inside atoms, the coupling with the electric field in the interstitial region, and the spin-orbit torque in ferromagnetic Fe, Co, and Ni metals. The calculated results show that the spin-orbit coupling is strong enough to cause enhancement of the minority-spin d electrons in these metals, which reduces the spin magnetic moment of the Co and Ni metals by 0.3764 mu(B) and 0.0619 mu(B), respectively. The z-component of the d-orbital orbital magnetic moments obtained are 0.0375 mu(B), 0.1323 mu(B), and 0.0628 mu(B), respectively, for the Fe, Co, and Ni metals. The calculated dependence of the Landau-Lifshitz damping coefficient, lambda, on the temperature has a similar trend as that of the experimental one in low temperatures. This study suggests that the low temperature Lorentzian broadening is not due to a temperature sensitive mechanism, but may be due to energy transfer or resonances with magnetic field induced degrees of freedom. The observed drop of lambda with the increase of temperature is found to be due to the increase of the chemical potential relative to the Fermi level.

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