On Guided Remagnetization in Layered Anoheterostructures

A. Korostil
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Abstract

Field-guided magnetic dynamics in magnetic multilayer nanostructures involves interconnection of the control field with localized spin states, which can occur directly or indirectly depending on the nature of the field and spin polarization. At the control electromagnetic field, this interconnection can be directly induced by the photon-induced spin-flip processes and indirectly by a bias field during antiferromagnetic exchange relaxation. The control impact of electric field and electric current on the magnetic states occurs indirectly via the spin polarization and spin current in combination with the exchange interaction of these polarized spins with localized magnetic states. The corresponding description of the magnetic dynamics is based on the modified Landau-Lifshitz equation and spin diffusion equations, taking into account the spin Hall and the inverse spin Hall effects for systems with normal metal sublayers. In the case of the magnetic nanostructures with the Rashba spin-orbit interaction in interfaces, the electric field-controlled magnetization is realized via the Rashba field-induced spin polarization, and its exchange interaction with localized magnetic states. Corresponding description is based on a tight-binding model of spin-orbit-coupled electrons exchange coupled to the localized magnetic states.
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层状异质结构的引导再磁化研究
磁多层纳米结构中的场引导磁动力学涉及控制场与局域自旋态的相互连接,这取决于场和自旋极化的性质,可以直接或间接地发生。在控制电磁场下,这种互连可以由光子诱导的自旋翻转过程直接诱导,也可以由反铁磁交换弛豫过程中的偏置场间接诱导。电场和电流对磁态的控制作用是通过自旋极化和自旋电流结合这些极化自旋与局域磁态的交换作用间接发生的。相应的磁动力学描述基于修正的Landau-Lifshitz方程和自旋扩散方程,考虑了正常金属子层体系的自旋霍尔效应和逆自旋霍尔效应。对于界面中存在Rashba自旋-轨道相互作用的磁性纳米结构,电场控制磁化是通过Rashba场诱导的自旋极化及其与局域磁态的交换相互作用实现的。相应的描述是基于耦合到局域磁态的自旋轨道耦合电子交换的紧密结合模型。
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