Doping a fractional quantum anomalous Hall insulator

TL;DR

This paper explores new itinerant phases emerging from doping fractional quantum anomalous Hall insulators, including topological superconductors, non-Abelian states, and charge density waves, revealing rich correlated phenomena beyond traditional models.

Contribution

It introduces a novel analytical framework for understanding doped FQAH insulators, predicting a variety of exotic itinerant phases with unique topological and superconducting properties.

Findings

Identification of topological superconductor with chiral edge modes

Prediction of a non-Abelian Pair Density Wave superconductor

Discovery of a doping-induced charge density wave and Fermi liquid states

Abstract

We study novel itinerant phases that can be accessed by doping a fractional quantum anomalous Hall (FQAH) insulator, with a focus on the experimentally observed Jain states at lattice filling $\nu = p/(2p+1)$. Unlike in the lowest Landau level, where charge motion is confined into cyclotron orbits, the charged excitations in the FQAH occupy Bloch states with well-defined crystal momenta. At a non-zero doping density, this enables the formation of itinerant states of the doped anyons just beyond the FQAH plateau region. Specializing to the vicinity of $\nu = 2/3$, we describe a few possible such itinerant states. These include a topological superconductor with chiral neutral fermion edge modes as well as a more exotic Pair Density Wave (PDW) superconductor with non-trivial non-Abelian topological order. A Fermi liquid metal with a doping-induced period-3 charge density wave also occurs naturally in our analysis. This Fermi liquid (as well as the PDW) arises from pairing instabilities of a composite Fermi liquid metal that can emerge near filling $2/3$. Though inspired by the theory of anyon superconductivity, we explain how our construction is qualitatively different. At a general Jain filling $\nu = p/(2p+1)$, the same analytical framework leads to a wider variety of phases including higher-charge superconductors and generalized composite Fermi liquids. We predict unusual physical signatures associated with each phase and analyze the crossover between different temperature regimes. These results provide a proof-of-principle that exotic itinerant phases can be stabilized by correlations intrinsic to the FQAH setup.