paper

Theory of Disordered Quantum Thermal Hall State: Emergent Symmetry and Phase Diagram

arXiv:1801.10149 · doi:10.1103/PhysRevB.97.165124

Abstract

Fractional quantum Hall (FQH) system at Landau level filling fraction has long been suggested to be non-Abelian, either Pfaffian (Pf) or antiPfaffian (APf) states by numerical studies, both with quantized Hall conductance . Thermal Hall conductances of the Pf and APf states are quantized at and respectively in a proper unit. However, a recent experiment shows the thermal Hall conductance of FQH state is . It has been speculated that the system contains random Pf and APf domains driven by disorders, and the neutral chiral Majorana modes on the domain walls may undergo a percolation transition to a phase. In this work, we do perturbative and non-perturbative analyses on the domain walls between Pf and APf. We show the domain wall theory possesses an emergent SO(4) symmetry at energy scales below a threshold , which is lowered to an emergent U(1)U(1) symmetry at energy scales between and a higher value , and is finally lowered to the composite fermion parity symmetry above . Based on the emergent symmetries, we propose a phase diagram of the disordered FQH system, and show that a phase arises at disorder energy scales . Furthermore, we show the gapped double-semion sector of compact domain walls contributes non-local topological degeneracy , causing a low-temperature peak in the heat capacity. We implement a non-perturbative method to bootstrap generic topological 1+1D domain walls (2-surface defects) applicable to any 2+1D non-Abelian topological order. We identify potentially relevant spin TQFTs for various FQH states in terms of fermionic version of U(1) Chern-Simons theory -class TQFTs.

44 pages, 9 figures, 3 tables. v2: Clarification/Refs added

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