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arXiv 0810.1340cond-mat.mes-hallcond-mat.str-el
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铁磁体中的横向自旋扩散

Transverse spin diffusion in ferromagnets

Yaroslav Tserkovnyak, E. M. Hankiewicz, Giovanni Vignale

摘要:

讨论了铁磁旋进的唯象Landau-Lifshitz方程中的耗散扩散项$\mathbf{m}\times\nabla^2\partial_t\mathbf{m}$,它描述了有限动量自旋波的增强Gilbert阻尼.这个术语在物理上来自于通过扰动铁磁配置的巡回电子自旋流,并且可以被理解为起源于连续极限中的铁磁自旋泵浦。我们开发了一个一般的现象学,以及提供微观理论的斯通纳和s-d模型的铁磁性,考虑到无序和电子-电子散射。后者在我们的问题中通过自旋带之间的库仑阻力表现出来。自旋扩散是根据横向自旋电导率确定的,类似于动力学理论中的爱因斯坦关系。

英文摘要:

We discuss the dissipative diffusion-type term of the form $\mathbf{m}\times\nabla^2\partial_t\mathbf{m}$ in the phenomenological Landau-Lifshitz equation of ferromagnetic precession, which describes enhanced Gilbert damping of finite-momentum spin waves. This term arises physically from itinerant-electron spin flows through a perturbed ferromagnetic configuration and can be understood to originate in the ferromagnetic spin pumping in the continuum limit. We develop a general phenomenology as well as provide microscopic theory for the Stoner and s-d models of ferromagnetism, taking into account disorder and electron-electron scattering. The latter is manifested in our problem through the Coulomb drag between the spin bands. The spin diffusion is identified in terms of the transverse spin conductivity, in analogy with the Einstein relation in the kinetic theory.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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