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Nonparabolicity effects and the spin-split electron dwell time in symmetric III-V double-barrier structures

机译:非对称性效应和对称III-V双势垒结构中的自旋分裂电子​​停留时间

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摘要

We start from the fourth order nonparabolic and anisotropic conduction band bulk dispersion relation to obtain an one-band effective Hamiltonian which we apply to an AlGaSb symmetric double-barrier structure with resonant energies significantly (more than 200meV) above the well bottom. The spin-splitting is described by the k3 Dresselhaus spin-orbit coupling term modifying only the effective mass of the spin eigenstates in the investigated structure. Apart from the bulk-like resonant energy shift due to the band nonparabolicity, we obtain a substantial shift depending on the choice of boundary conditions for the envelope functions at interfaces between different materials. The shift of resonant energy levels leads to the change of spin-splitting and the magnitude of the dwell times. We attempt to explain the influence of both the nonparabolicity and boundary conditions choice by introducing various effective masses.ud
机译:我们从四阶非抛物线和各向异性的导带整体散布关系开始,获得一个单带有效哈密顿量,该哈密顿量适用于在井底上方具有明显共振能量(大于200meV)的AlGaSb对称双势垒结构。自旋分裂由k3 Dresselhaus自旋轨道耦合项描述,它仅修改了所研究结构中自旋本征态的有效质量。除了由于带的非抛物线性引起的块状共振能移动以外,我们还根据不同材料之间界面处的包络函数的边界条件的选择获得了实质性的移动。共振能级的移动会导致自旋分裂和停留时间的大小发生变化。我们试图通过引入各种有效质量来解释非抛物线性和边界条件选择的影响。 ud

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