Localization – Weak Antilocalization Crossover in Two-Dimensional Materials with Spin-Orbit Interaction

U. A. Zaitsau, D. A. Podryabinkin, V. V. Melnikova, A. L. Danilyuk, S. L. Prischepa
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Abstract

In this paper, the patterns of manifestation of weak localization and antilocalization in graphene with enhanced spin-orbit interaction, as well as in a topological insulator with a gap in surface states induced by magnetic impurities are studied. The parameters characterizing the manifestation of weak localization, antilocalization and crossover between them are established. Quantum corrections to the conductivity of graphene are determined in units of e 2 /h = 38.64 μS for various ratios between the characteristic dephasing time and spin-orbit scattering time. It has been established that with a relatively long spin-orbit scattering time, not less than 10 –10 s, it does not affect the correction to conductivity and its value is determined by the dephasing time and the times of intervalley and intravalley scattering. The effect of the spin-orbit scattering is to suppress weak antilocalization. It leads to a spin flip of the conduction electron during elastic scattering, and the interference pattern of weak localization becomes more complicated due to the mixing of spin states. The sign of the quantum correction depends on which spin state contributes the most.
自旋-轨道相互作用下二维材料的局部化-弱反局部化交叉
本文研究了自旋轨道相互作用增强的石墨烯中弱局域化和反局域化的表现模式,以及磁性杂质诱导的具有表面态间隙的拓扑绝缘体中弱局域化和反局域化的表现模式。建立了表征弱局域化、反局域化和它们之间交叉表现的参数。在特征失相时间和自旋轨道散射时间的不同比例下,以e2 /h = 38.64 μS为单位确定了石墨烯电导率的量子修正。在较长的自旋轨道散射时间(不小于10 -10 s)下,不影响电导率校正,其值由消相时间、谷间散射次数和槽内散射次数决定。自旋轨道散射的作用是抑制弱反局域化。在弹性散射过程中,导电子发生自旋翻转,由于自旋态的混合,弱局域化的干涉图变得更加复杂。量子修正的符号取决于哪个自旋态贡献最大。
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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