The Quantum Hall Fluid and Non-Commutative Chern Simons Theory
L. Susskind (Stanford U.)

TL;DR
This paper reviews the Chern-Simons approach to the Quantum Hall effect, proposes an equivalence with non-commutative Chern-Simons theory at certain levels, and explores its formulation as a matrix and mapping theory.
Contribution
It demonstrates the exact equivalence between abelian non-commutative Chern-Simons theory at level n and Laughlin's theory at filling fraction 1/n, and connects it to matrix and non-commutative space theories.
Findings
Non-commutative Chern-Simons theory is equivalent to Laughlin theory at 1/n.
The theory can be formulated as a matrix model similar to D0-branes.
It can be viewed as a quantum mapping between non-commutative spaces.
Abstract
The first part of this paper is a review of the author's work with S. Bahcall which gave an elementary derivation of the Chern Simons description of the Quantum Hall effect for filling fraction . The notation has been modernized to conform with standard gauge theory conventions. In the second part arguments are given to support the claim that abelian non-commutative Chern Simons theory at level is exactly equivalent to the Laughlin theory at filling fraction . The theory may also be formulated as a matrix theory similar to that describing D0-branes in string theory. Finally it can also be thought of as the quantum theory of mappings between two non-commutative spaces, the first being the target space and the second being the base space.
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Taxonomy
TopicsBlack Holes and Theoretical Physics · Noncommutative and Quantum Gravity Theories · Algebraic structures and combinatorial models
