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Landau Levels and Edge States in Graphene with Strong Spin-Orbit Coupling

机译:强自旋轨道耦合的石墨烯中的朗道能级和边缘态

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We investigate the electronic properties of graphene in a magnetic and a strain-induced pseudo-magnetic field in the presence of strong spin-orbit interactions (SOI). For a homogeneous field we provide analytical results for the Landau level eigenstates for arbitrary intrinsic and Rashba SOI, including also the effect of a Zeeman field. We then study the edge states in a semi-infinite geometry in the absence of the Rashba term. We find that, for a critical value of the magnetic field, a quantum phase transition occurs, which separates two phases both with spin-filtered helical edge states but with opposite direction of the spin current. Finally,we discuss magnetic waveguides with inhomogeneous field profiles that allow for chiral snake orbits. Such waveguides are practically immune to disorder-induced backscattering, and the SOI provides non-trivial spin texture to these modes.
机译:我们在强自旋轨道相互作用(SOI)的存在下,在磁场和应变诱导的伪磁场中研究石墨烯的电子性质。对于均匀场,我们提供了针对任意固有和Rashba SOI的Landau能级本征态的分析结果,还包括塞曼场的影响。然后,我们在没有Rashba项的情况下研究半无限几何形状中的边缘状态。我们发现,对于磁场的临界值,发生量子相变,该量子相变将具有自旋滤波的螺旋边缘状态但具有与自旋电流相反的方向的两个相分离。最后,我们讨论了具有不均匀场分布的电磁波导管,它们允许手性蛇形轨道。这样的波导实际上不受无序引起的反向散射的影响,SOI为这些模式提供了非平凡的自旋纹理。

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  • 会议地点 Tashkent(UZ)
  • 作者单位

    Department of Mathematical Science, City University London, Northampton Square, London EC1V 0HB.UK;

    Institut fur Theoretische Physik, Heinrich-Heine-Universit, D-40225 Duesseldorf, Germany;

    Institut fuer Theoretische Physik, Heinrich-Heine-Universit, D-40225 Duesseldorf, Germany;

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