Localization of the Helical Edge States in the Absense of External Magnetic Field

Theoretically, the helical edge states of two-dimensional topological insulators are protected from coherent backscattering due to nonmagnetic disorder provided electron interactions are not too strong. Experimentally, the edges typically do not demonstrate the systematic and robust quantization, at...

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Bibliographic Details
Published in:arXiv.org 2021-04
Main Authors: Bubis, A V, Mikhailov, N N, Dvoretsky, S A, Nasibulin, A G, Tikhonov, E S
Format: Article
Language:English
Subjects:
Backscattering
Localization
Magnetic fields
Magnetoresistance
Magnetoresistivity
Micrometers
Quantum wells
Topological insulators
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Summary:Theoretically, the helical edge states of two-dimensional topological insulators are protected from coherent backscattering due to nonmagnetic disorder provided electron interactions are not too strong. Experimentally, the edges typically do not demonstrate the systematic and robust quantization, at the same time little is known about the sub-Kelvin temperature behavior. Here, we report the surprising localization of the edge states in an 8 nm HgTe quantum well in zero magnetic field at millikelvin temperatures. Additionally, the magnetoresistance data at 0.5 K for the edges few micrometers long suggests the field-dependent localization length \(l_B\propto B^{-\alpha}\), with \(\alpha\) ranging approximately from \(1.6\) to \(2.8\) at fields \(B\lesssim0.1\,\text{T}\) and \(\alpha\approx1.1\) at higher fields up to \(0.5\,\text{T}\). In the frame of disordered interacting edge, these values of \(\alpha\) correspond to the Luttinger liquid parameters \(K\approx 0.9-1.1\) and \(K\approx 0.6\), respectively. We discuss possible scenarios which could result in the zero magnetic field localization.
ISSN:2331-8422
DOI:10.48550/arxiv.2104.13300