Spin and charge transport induced by gauge fields in a ferromagnet
arXiv:1107.2165 · doi:10.1103/PhysRevB.84.184408
Abstract
We present a microscopic theory of spin-dependent motive force ("spin motive force") induced by magnetization dynamics in a conducting ferromagnet, by taking account of spin relaxation of conduction electrons. The theory is developed by calculating spin and charge transport driven by two kinds of gauge fields; one is the ordinary electromagnetic field , and the other is the effective gauge field induced by dynamical magnetic texture. The latter acts in the spin channel and gives rise to a spin motive force. It is found that the current induced as a linear response to is not gauge-invariant in the presence of spin-flip processes. This fact is intimately related to the non-conservation of spin via Onsager reciprocity, so is robust, but indicates a theoretical inconsistency. This problem is resolved by considering the time dependence of spin-relaxation source terms in the "rotated frame", as in the previous study on Gilbert damping [J. Phys. Soc. Jpn. {\bf 76}, 063710 (2007)]. This effect restores the gauge invariance while keeping spin non-conservation. It also gives a dissipative spin motive force expected as a reciprocal to the dissipative spin torque ("-term").
13 pages, 3 figures, submitted to PRB
References in corpus (11)
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- Energetic perspective on emergent inductance exhibited by magnetic textures in the pinned regime
- Spin-motive force due to domain wall motion in the presence of Dzyaloshinskii-Moriya Interaction
- Stability of Spinmotive Force in Perpendicularly Magnetized Nanowires under High Magnetic Fields
- Variational approach to the stationary spin-Hall effect
- Coupling theory of emergent spin electromagnetic field and electromagnetic field
- Spin torque due to diffusive spin current in magnetic texture
- Stationary states and screening equations in the spin-Hall effect