Finite-wave-vector electromagnetic response of fractional quantized Hall states

Steven H. Simon and Bertrand I. Halperin
Phys. Rev. B 48, 17368 – Published 15 December 1993
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Abstract

A fractional quantized Hall state with filling fraction ν=p/(2mp+1) can be modeled as an integer quantized Hall state of transformed fermions, interacting with a Chern-Simons field. The electromagnetic response function for these states at arbitrary frequency and wave vector can be calculated using a semiclassical approximation or the random-phase approximation. However, such calculations do not properly take into account the large effective-mass renormalization which is present in the Chern-Simons theory. We show how the mass renormalization can be incorporated in a calculation of the response function within a Landau-Fermi-liquid theory approach such that Kohn’s theorem and the f-sum rules are properly satisfied. We present results of such calculations.

  • Received 16 July 1993

DOI:https://doi.org/10.1103/PhysRevB.48.17368

©1993 American Physical Society

Authors & Affiliations

Steven H. Simon and Bertrand I. Halperin

  • Physics Department, Harvard University, Cambridge, Massachusetts 02138

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Vol. 48, Iss. 23 — 15 December 1993

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