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首页> 外文期刊>Physical review. B, Condensed Matter And Materials Physics >Spin-polarized electron transport in ferromagnet/semiconductor heterostructures: Unification of ballistic and diffusive transport
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Spin-polarized electron transport in ferromagnet/semiconductor heterostructures: Unification of ballistic and diffusive transport

机译:铁磁体/半导体异质结构中的自旋极化电子传输:弹道和扩散传输的统一

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摘要

A theory of spin-polarized electron transport in ferromagnet/semiconductor heterostructures, based on a unified semiclassical description of ballistic and diffusive transport in semiconductor structures, is developed. The aim is to provide a comprehensive framework for systematically studying the interplay of spin relaxation and transport mechanism in spintronic devices. A key element of the unified description of transport inside a (nondegenerate) semiconductor is the thermoballistic current consisting of electrons which move ballistically in the electric field arising from internal and external electrostatic potentials, and which are thermalized at randomly distributed equilibration points. The ballistic component in the unified description gives rise to discontinuities in the chemical potential at the boundaries of the semiconductor, which are related to the Sharvin interface conductance. By allowing spin relaxation to occur during the ballistic motion between the equilibration points, a thermoballistic spin-polarized current and density are constructed in terms of a spin transport function. An integral equation for this function is derived for arbitrary profile of the electrostatic potential and for arbitrary values of the momentum and spin relaxation lengths. Detailed consideration is given to field-driven spin-polarized transport in a homogeneous semiconductor. An approximation is introduced which allows one to convert the integral equation into a second-order differential equation that generalizes the standard spin drift-diffusion equation. The spin polarization in ferromagnet/semiconductor heterostructures is obtained by invoking continuity of the current spin polarization and matching the spin-resolved chemical potentials on the ferromagnet sides of the interfaces. Allowance is made for spin-selective interface resistances. Examples are considered that illustrate the effects of transport mechanism and electric field.
机译:提出了一种基于铁磁/半导体异质结构中自旋极化电子输运的理论,该理论基于对半导体结构中弹道和扩散输运的统一半经典描述。目的是为系统研究自旋电子器件中自旋弛豫和传输机制的相互作用提供一个全面的框架。统一描述(非退化的)半导体内部传输的关键要素是由电子组成的热弹道电流,这些电子在由内部和外部静电势产生的电场中弹道运动,并在随机分布的平衡点处被热化。统一描述中的弹道成分会导致半导体边界处化学势的不连续,这与Sharvin界面电导有关。通过在平衡点之间的弹道运动期间发生自旋弛豫,就自旋输运函数构造了热弹自旋极化电流和密度。对于静电势的任意分布以及动量和自旋弛豫长度的任意值,可以导出此函数的积分方程。详细考虑了均匀半导体中场驱动的自旋极化传输。引入一个近似值,该近似值允许将积分方程式转换为可推广标准自旋漂移扩散方程式的二阶微分方程式。铁磁性/半导体异质结构中的自旋极化是通过调用电流自旋极化的连续性并使界面的铁磁体侧上的自旋分辨化学势匹配而获得的。为自旋选择界面电阻留有余地。认为例子说明了传输机制和电场的影响。

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