Lowest-Landau-level theory of the quantum Hall effect: The Fermi-liquid-like state of bosons at filling factor one

Abstract

A theory for a Fermi-liquid-like state in a system of charged bosons at filling factor 1 is developed, working in the lowest Landau level. The approach is based on a representation of the problem as fermions with a system of constraints, introduced by Pasquier and Haldane (unpublished). This makes the system a gauge theory with gauge algebra ${W}_{\ensuremath{\infty}}.$ The low-energy theory is analyzed based on a Hartree-Fock approximation and a corresponding conserving approximation. This is shown to be equivalent to introducing a gauge field, which at long wavelengths gives an infinite-coupling U(1) gauge theory, without a Chern-Simons term. The system is compressible, and the Fermi-liquid properties are similar, but not identical, to those in the previous U(1) Chern-Simons fermion theory. The fermions in the theory are effectively neutral, but carry a dipole moment. The density-density response, longitudinal conductivity, and current density are considered explicitly.