Spin segregation of nonrelativistic charged particles by a helical magnetic field slab.

D Martínez, J A Reyes, A Lima
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引用次数: 0

Abstract

We study a beam of nonrelativistic spin-charge carriers incident normally on a finite slab of helical magnetic field aligned along the beam axis. Starting from the Pauli-Schrödinger equation, we apply a unitary transformation expressed in terms of Pauli matrices to map the system to a spatially independent eigenvalue problem, from which the energy band structure is obtained analytically. Our results reveal two types of bandgap controlled by the field strength: a partial bandgap present for all field values, in which only one spin channel propagates, and a total bandgap that opens above a threshold field strength, in which both channels are evanescent. Using the eigenvectors and a transfer matrix approach, we solve the boundary value problem at the vacuum-magnetic interface and obtain spin-preserving and spin-flip transmittances and reflectances as functions of field strength and energy. The spin-filtering properties are discussed in terms of the alignment of the spin eigenstates with the effective field in spin space, with the Bloch sphere providing a geometric picture of the spin-channel selection mechanism.

非相对论性带电粒子在螺旋磁场板上的自旋偏析。
我们研究了一束非相对论自旋载流子正常入射到沿束流轴排列的有限螺旋磁场板上。从泡利—Schrödinger方程出发,应用以泡利矩阵表示的酉变换将系统映射为空间无关的特征值问题,并由此解析得到能量 ;带结构。我们的研究结果揭示了由场强控制的两种类型的带隙:所有场值都存在部分带隙,其中只有一个自旋通道传播,以及在阈值场强以上打开的总带隙,其中两个通道都消失。利用本征向量和传递矩阵方法,求解了真空-磁界面边值问题,得到了保持自旋和翻转自旋的透射率和反射率随场强和能量的函数。从自旋本征态与有效场在自旋空间中的对齐角度讨论了自旋滤波特性,并用Bloch球提供了自旋通道选择机制的几何图像。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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