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Band structure and magnetotransport of a two-dimensional electron gas in the presence of spin-orbit interaction

机译:自旋轨道相互作用下二维电子气的能带结构和磁输运

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摘要

The band structure and magnetotransport of a two-dimensional electron gas (2DEG), in the presence of the Rashba (RSOI) and Dresselhaus (DSOI) terms of the spin-orbit interaction and of a perpendicular magnetic field, is investigated. Exact and approximate analytical expressions for the band structure are obtained quantum mechanically and used to calculate the density of states (DOS) and the longitudinal magnetoresitivity assuming a Gaussian type of level broadening. The interplay between the Zeeman coupling and the two terms of the SOI is discussed. If the strengths α and β, of the RSOI and DSOI, respectively, are equal and the g factor vanishes, the two spin states are degenerate and a shifted Landau-level structure appears in agreement with recent semiclassical results. With the increase of the difference α-β, a beating pattern of the DOS and of the Shubnikov-de Haas oscillations appears distinctly different from that occurring when one of these strengths vanishes. For α β or α β the peaks in one wrap of the beating pattern occur at even filling factors of the 2DEG while in the next wrap they occur at odd filling factors. For α≈β this transition occurs only if the spin splitting is larger than half the Landau energy.
机译:研究了存在自旋轨道相互作用和垂直磁场的Rashba(RSOI)和Dresselhaus(DSOI)项下的二维电子气(2DEG)的能带结构和磁输运。通过量子力学获得能带结构的精确和近似解析表达式,并假设高斯类型的能级展宽,将其用于计算态密度(DOS)和纵向磁电阻率。讨论了Zeeman耦合和SOI的两个术语之间的相互作用。如果RSOI和DSOI的强度α和β分别相等,并且g因子消失,则两个自旋态简并,并且出现移位的Landau能级结构与最近的半经典结果一致。随着差值α-β的增加,DOS和Shubnikov-de Haas振荡的跳动模式与这些强度之一消失时出现的跳动模式明显不同。对于αβ或αβ,在2DEG的偶数填充因子处出现一个搏动模式的峰,而在下一个包裹中,它们以奇数填充因数出现。对于α≈β,仅当自旋分裂大于Landau能量的一半时,才会发生此跃迁。

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