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Quantum Interference Effects in Topological Nanowires In a Longitudinal Magnetic Field

机译:拓扑纳米线在纵向上的量子干涉效应   磁场

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摘要

We study the magnetoconductance of topological insulator nanowires in alongitudinal magnetic field, including Aharonov-Bohm, Altshuler-Aronov-Spivak,perfectly conducting channel, and universal conductance fluctuation effects.Our focus is on predicting experimental behavior in single wires in the quantumlimit where temperature is reduced to zero. We show that changing the Fermienergy $E_F$ can tune a wire from from ballistic to diffusive conduction and tolocalization. In both ballistic and diffusive single wires we find bothAharonov-Bohm and Altshuler-Aronov-Spivak oscillations with similar strengths,accompanied by quite strong universal conductance fluctuations (UCFs), all withamplitudes between $0.3 \, G_0$ and $1\,G_0$. This contrasts strongly with theaverage behavior of many wires, which shows Aharonov-Bohm oscillations in theballistic regime and Altshuler-Aronov-Spivak oscillations in the diffusiveregime, with both oscillations substantially larger than the conductancefluctuations. In single wires the ballistic and diffusive regimes can bedistinguished by varying $E_F$ and studying the sign of the AB signal, whichdepends periodically on $E_F$ in ballistic wires and randomly on $E_F$ indiffusive wires. We also show that in long wires the perfectly conductingchannel is visible at a wide range of energies within the bulk gap. We presenttypical conductance profiles at several wire lengths, showing that conductancefluctuations can dominate the average signal. Similar behavior will be found incarbon nanotubes.
机译:我们研究了拓扑绝缘体纳米线在纵向磁场(包括Aharonov-Bohm,Altshuler-Aronov-Spivak),完美导电通道和通用电导波动效应中的磁导率。我们的研究重点是在温度为量子极限的单线中预测实验行为减少到零。我们表明,改变费米能量$ E_F $可以将导线从弹道调整为扩散传导和局部化。在弹道和扩散单线中,我们都发现了具有相似强度的Aharonov-Bohm和Altshuler-Aronov-Spivak振荡,并伴随着相当强的通用电导涨落(UCF),所有振幅都在$ 0.3 \,G_0 $和$ 1 \,G_0 $之间。这与许多导线的平均行为形成鲜明对比,后者显示出弹道状态下的Aharonov-Bohm振荡和扩散状态下的Altshuler-Aronov-Spivak振荡,这两种振荡都远大于电导波动。在单线中,可以通过改变$ E_F $并研究AB信号的符号来区分弹道和扩散状态,该信号周期性地取决于弹道线中的$ E_F $和随机地取决于$ E_F $扩散线。我们还表明,在长导线中,在整个间隙内的各种能量范围内都可以看到完美的导电通道。我们给出了几种导线长度的典型电导曲线,表明电导波动可以控制平均信号。在碳纳米管中会发现类似的行为。

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