Non-diagonal anisotropic quantum Hall states

TL;DR

This paper introduces a new family of Abelian quantum Hall states called non-diagonal states, characterized by unique symmetry-enriched topological orders, constructed via coupled wire models, and distinguished by their interplay of charge and translation symmetries.

Contribution

The paper constructs and characterizes non-diagonal quantum Hall states with novel symmetry properties and provides a microscopic derivation of their boundary theories, highlighting their distinction from traditional states.

Findings

Non-diagonal states occur at specific filling factors for bosons and fermions.

These states exhibit a symmetry-enriched topological order with a neutral sector described by quantum double models.

Edge theories include a chiral Luttinger liquid and a generalized clock model, with translation symmetry acting as self-duality.

Abstract

We propose a family of Abelian quantum Hall states termed the non-diagonal states, which arise at filling factors $\nu=p/2q$ for bosonic systems and $\nu=p/(p+2q)$ for fermionic systems, with $p$ and $q$ being two coprime integers. Non-diagonal quantum Hall states are constructed in a coupled wire model, which shows an intimate relation to the non-diagonal conformal field theory and has a constrained pattern of motion for bulk quasiparticles, featuring a non-trivial interplay between charge symmetry and translation symmetry. The non-diagonal state is established as a distinctive symmetry-enriched topological order. Aside from the usual $U(1)$ charge sector, there is an additional symmetry-enriched neutral sector described by the quantum double model $\mathcal{D}(\mathbb{Z}_p)$, which relies on the presence of both the $U(1)$ charge symmetry and the $\mathbb{Z}$ translation symmetry of the wire model. Translation symmetry distinguishes non-diagonal states from Laughlin states, in a way similar to how it distinguishes weak topological insulators from trivial band insulators. Moreover, the translation symmetry in non-diagonal states can be associated to the $\mathbf{e}\leftrightarrow\mathbf{m}$ anyonic symmetry in $\mathcal{D}(\mathbb{Z}_p)$, implying the role of dislocations as two-fold twist-defects. The boundary theory of non-diagonal states is derived microscopically. For the edge perpendicular to the direction of wires, the effective Hamiltonian has two components: a chiral Luttinger liquid and a generalized $p$-state clock model. Importantly, translation symmetry in the bulk is realized as self-duality on the edge. The symmetric edge is thus either gapless or gapped with spontaneously broken symmetry. For $p=2,3$, the respective electron tunneling exponents are predicted for experimental probes.