paper

Symmetric localization of fractional topological insulator edges

arXiv:2603.10103 · doi:10.1103/gcpg-wf17

Abstract

Motivated by the recent twisted MoTe experiment [arXiv:2601.18508], we develop a disordered interacting edge theory of a fractional topological insulator at , consisting of two time-reversal-conjugated fractional quantum Hall states. For an -conserving edge, we uncover three distinct phases with two possible conductance values per edge in the long-edge limit: and . In the presence of -changing perturbations (e.g., Rashba spin-orbit coupling), an interaction-induced insulating edge state can emerge without breaking time-reversal or charge-conservation symmetry, corresponding to the absence of a topologically protected edge state. We show an exact mapping (with a special choice of parameters) to a noninteracting fermionic theory exhibiting Anderson localization, and the weak-coupling phase diagrams are also constructed, showing that symmetric localization can emerge regardless of other -conserving perturbations. Our results showcase an explicit, experimentally relevant example that the edge-state two-terminal transport can yield false-negative results in identifying the fractional topological insulators.

9 pages, 2 figures; published version

References in corpus (27)