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Electronic structure of paramagnetic In1-xMnx as nanowires

机译:顺磁性In1-xMnx作为纳米线的电子结构

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The electronic structure, spin splitting energies, and g factors of paramagnetic In1-xMnxAs nanowires under magnetic and electric fields are investigated theoretically including the sp-d exchange interaction between the carriers and the magnetic ion. We find that the effective g factor changes dramatically with the magnetic field. The spin splitting due to the sp-d exchange interaction counteracts the Zeeman spin splitting. The effective g factor can be tuned to zero by the external magnetic field. There is also spin splitting under an electric field due to the Rashba spin-orbit coupling which is a relativistic effect. The spin-degenerated bands split at nonzero k(z) (k(z) is the wave vector in the wire direction), and the spin-splitting bands cross at k(z) = 0, whose k(z)-positive part and negative part are symmetrical. A proper magnetic field makes the k(z)-positive part and negative part of the bands asymmetrical, and the bands cross at nonzero k(z). In the absence of magnetic field, the electron Rashba coefficient increases almost linearly with the electric field, while the hole Rashba coefficient increases at first and then decreases as the electric field increases. The hole Rashba coefficient can be tuned to zero by the electric field.
机译:理论上研究了顺磁性In1-xMnxAs纳米线在磁场和电场下的电子结构,自旋分裂能和g因子,包括载流子与磁性离子之间的sp-d交换相互作用。我们发现有效的g因子随磁场变化很大。由于sp-d交换相互作用而引起的自旋分裂抵消了塞曼自旋分裂。有效的g因子可以通过外部磁场调整为零。由于Rashba自旋轨道耦合,在电场作用下也会发生自旋分裂,这是相对论的效应。自旋简并谱带在非零k(z)处分裂(k(z)是导线方向上的波矢量),并且自旋分裂谱带在k(z)= 0处交叉,其k(z)为正和负部分是对称的。适当的磁场会使频段的k(z)正部分和负部分不对称,并且频段在非零k(z)处交叉。在没有磁场的情况下,电子拉什巴系数几乎随电场线性增加,而空穴拉什巴系数首先增加,然后随电场增加而减小。可以通过电场将空穴的拉什巴系数调整为零。

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