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

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Xypakis,  Emmanouil
Max Planck Institute for the Physics of Complex Systems, Max Planck Society;

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Bardarson,  Jens H.
Max Planck Institute for the Physics of Complex Systems, Max Planck Society;

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Citation

Dufouleur, J., Veyrat, L., Dassonneville, B., Xypakis, E., Bardarson, J. H., Nowka, C., et al. (2017). Weakly-coupled quasi-1D helical modes in disordered 3D topological insulator quantum wires. Scientific Reports, 7: 45276. doi:10.1038/srep45276.


Cite as: https://hdl.handle.net/11858/00-001M-0000-002D-A3A8-C
Abstract
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. of such modes is much smaller than their energy spacing., 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 spinhelical 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.