Gapless insulating edges of dirty interacting topological insulators
arXiv:1710.04232 · doi:10.1103/PhysRevB.98.054205
Abstract
We demonstrate that a combination of disorder and interactions in a two-dimensional bulk topological insulator can generically drive its helical edge insulating. We establish this within the framework of helical Luttinger liquid theory and exact Emery-Luther mapping. The gapless glassy edge state spontaneously breaks time-reversal symmetry in a `spin glass' fashion, and may be viewed as a localized state of solitons which carry half integer charge. Such a qualitatively distinct edge state provides a simple explanation for heretofore puzzling experimental observations. This phase exhibits a striking non-monotonicity, with the edge growing less localized in both the weak and strong disorder limits.
6+6 pages and 5 figures, published version
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Cited by in corpus (23)
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- Helical Liquids in Semiconductors
- Low-Temperature Conductivity of Weakly Interacting Quantum Spin Hall Edges in Strained-Layer InAs/GaInSb
- Current-induced gap opening in interacting topological insulator surfaces
- Charge density wave and finite-temperature transport in minimally twisted bilayer graphene
- Localization of Extended Quantum Objects
- Anomalous localization at the boundary of an interacting topological insulator
- Localization-Driven Correlated States of Two Isolated Interacting Helical Edges
- Temperature-driven gapless topological insulator
- Theory of coherent phase modes in insulating Josephson junction arrays
- Composite helical edges from Abelian fractional topological insulators
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- Robustness of Helical Edge States Under Edge Reconstruction
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- Edge Reconstruction in a Quantum Spin Hall Insulator
- Symmetric localization of fractional topological insulator edges