Hall viscosity and geometric response in the Chern-Simons matrix model of the Laughlin states

TL;DR

This paper investigates the geometric response of Laughlin fractional quantum Hall states using the Chern-Simons matrix model, showing it captures guiding center contributions to Hall viscosity and related properties.

Contribution

The study demonstrates that the Chern-Simons matrix model accurately describes guiding center aspects of Laughlin states' geometric response, including Hall viscosity, but omits Landau orbit contributions.

Findings

CSMM captures guiding center contribution to Hall viscosity

CSMM reproduces geometric response in Laughlin states

Landau orbit contributions are absent in CSMM

Abstract

We study geometric aspects of the Laughlin fractional quantum Hall (FQH) states using a description of these states in terms of a matrix quantum mechanics model known as the Chern-Simons matrix model (CSMM). This model was proposed by Polychronakos as a regularization of the noncommutative Chern-Simons theory description of the Laughlin states proposed earlier by Susskind. Both models can be understood as describing the electrons in a FQH state as forming a noncommutative fluid, i.e., a fluid occupying a noncommutative space. Here we revisit the CSMM in light of recent work on geometric response in the FQH effect, with the goal of determining whether the CSMM captures this aspect of the physics of the Laughlin states. For this model we compute the Hall viscosity, Hall conductance in a non-uniform electric field, and the Hall viscosity in the presence of anisotropy (or intrinsic geometry). Our calculations show that the CSMM captures the guiding center contribution to the known values of these quantities in the Laughlin states, but lacks the Landau orbit contribution. The interesting correlations in a Laughlin state are contained entirely in the guiding center part of the state/wave function, and so we conclude that the CSMM accurately describes the most important aspects of the physics of the Laughlin FQH states, including the Hall viscosity and other geometric properties of these states which are of current interest.