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Weakly-coupled quasi-1D helical modes in disordered 3D topological insulator quantum wires

机译:3D拓扑绝缘子量子线中的弱耦合准1D螺旋模

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摘要

Disorder remains a key limitation in the search for robust signatures of topological superconductivity in condensed matter. Whereas clean semiconducting quantum wires gave promising results discussed in terms of Majorana bound states, disorder makes the interpretation more complex. Quantum wires of 3D topological insulators offer a serious alternative due to their perfectly-transmitted mode. An important aspect to consider is the mixing of quasi-1D surface modes due to the strong degree of disorder typical for such materials. Here, we reveal that the energy broadening γ of such modes is much smaller than their energy spacing Δ, an unusual result for highly-disordered mesoscopic nanostructures. This is evidenced by non-universal conductance fluctuations in highly-doped and disordered Bi2Se3 and Bi2Te3 nanowires. Theory shows that such a unique behavior is specific to spin-helical Dirac fermions with strong quantum confinement, which retain ballistic properties over an unusually large energy scale due to their spin texture. Our result confirms their potential to investigate topological superconductivity without ambiguity despite strong disorder.
机译:在寻找凝聚态拓扑超导性的可靠特征时,无序仍然是关键限制。干净的半导体量子线给出了根据马约拉纳结合态进行讨论的有希望的结果,而无序使解释变得更加复杂。 3D拓扑绝缘体的量子线由于其完美的传输模式而提供了一种严肃的替代方法。要考虑的一个重要方面是由于此类材料的典型无序程度高而导致准一维表面模式的混合。在这里,我们揭示了这种模式的能量扩展γ远小于它们的能量间隔Δ,这对于高度无序的介观纳米结构是不寻常的结果。高掺杂和无序的Bi2Se3和Bi2Te3纳米线的非普遍电导波动可以证明这一点。理论表明,这种独特的行为是具有强量子约束的自旋螺旋狄拉克费米子所特有的,由于其自​​旋结构,它们在异常大的能量范围内仍具有弹道特性。我们的结果证实了他们有潜力研究拓扑超导性,尽管存在很强的混乱性,但也不会产生歧义。

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