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Nonadiabatic spin-transfer torque in real materials

2008/12/13 by Ion Garate, K. Gilmore, Keith Gilmore +2 · 7 citations
Physics and Astronomy · #Adiabatic process #BETA (programming language) #Classical mechanics #Computer science #Condensed matter physics #Current (fluid) #Dimensionless quantity #Domain wall (magnetism) #Magnetic field #Magnetic properties of thin films #Magnetization #Physics #Physics of Superconductivity and Magnetism #Quantum and electron transport phenomena #Quantum mechanics #Spin (aerodynamics) #Spin-transfer torque #Thermodynamics #Torque #cond-mat.mtrl-sci

paper · pdf · doi:10.1103/physrevb.79.104416

published as Phys. Rev. B 79, 104416 (2009) · 18 pages, 9 figures; submitted to Phys. Rev. B

arxiv created 2008/12/13 · openalex publication_date 2009/03/16 · arxiv updated 2010/04/28 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05

Abstract

The motion of simple domain walls and of more complex magnetic textures in the presence of a transport current is described by the Landau-Lifshitz-Slonczewski (LLS) equations. Predictions of the LLS equations depend sensitively on the ratio between the dimensionless material parameter \ensuremathβ which characterizes nonadiabatic spin-transfer torques and the Gilbert damping parameter \ensuremathα. This ratio has been variously estimated to be close to zero, close to one, and large compared to one. By identifying \ensuremathβ as the influence of a transport current on \ensuremathα, we derive a concise, explicit, and relatively simple expression which relates \ensuremathβ to the band structure and Bloch state lifetimes of a magnetic metal. Using this expression we demonstrate that intrinsic spin-orbit interactions lead to intraband contributions to \ensuremathβ which are often dominant, and can be (i) estimated with some confidence and (ii) interpreted using the ``breathing Fermi-surface'' model.

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