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Transport in selectively magnetically doped topological insulator wires

机译:在选择性磁掺杂拓扑绝缘子导线中传输

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We study the electronic and transport properties of a topological insulator nanowire including selective magnetic doping of its surfaces. We use a model which is appropriate to describe materials like Bi_2Se_3 within a k · p approximation and consider nanowires with a rectangular geometry. Within this model the magnetic doping at the (111) surfaces induces a Zeeman field which opens a gap at the Dirac cones corresponding to the surface states. For obtaining the transport properties in a two terminal configuration we use a recursive Green's function method based on a tight-binding model which is obtained by discretizing the original continuous model. For the case of uniform magnetization of two opposite nanowire (111) surfaces we show that the conductance can switch from a quantized value of e~2/h (when the magnetizations are equal) to a very small value (when they are opposite). We also analyze the case of nonuniform magnetizations in which the Zeeman field on the two opposite surfaces change sign at the middle of the wire. For this case we find that conduction by resonant tunneling through a chiral state bound at the middle of the wire is possible. The resonant level position can be tuned by imposing an Aharonov-Bohm flux through the nanowire cross section.
机译:我们研究了拓扑绝缘体纳米线的电子和传输特性,包括其表面的选择性磁掺杂。我们使用一个模型来描述在k·p近似范围内的Bi_2Se_3等材料,并考虑具有矩形几何形状的纳米线。在该模型中,(111)表面的磁性掺杂会产生一个塞曼场,该场在Dirac锥上打开一个与表面状态相对应的间隙。为了获得两个终端配置中的传输特性,我们使用基于紧密绑定模型的递归格林函数方法,该方法是通过离散化原始连续模型而获得的。对于两个相对的纳米线(111)表面均匀磁化的情况,我们表明电导可以从e〜2 / h的量化值(当磁化强度相等时)切换到很小的值(当它们相反时)。我们还分析了非均匀磁化的情况,其中两个相对表面上的塞曼场改变了导线中间的符号。对于这种情况,我们发现通过共振隧穿穿过导线中部的手性态进行传导是可能的。可以通过施加穿过纳米线横截面的Aharonov-Bohm通量来调整共振能级位置。

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