Finite-temperature behavior of the ν=1 quantum Hall effect in bilayer electron systems

M. Abolfath, Ramin Golestanian, and T. Jungwirth
Phys. Rev. B 61, 4762 – Published 15 February 2000
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Abstract

An effective field theoretic description of ν=1 bilayer electron systems stabilized by Coulomb repulsion in a single wide quantum well is examined using renormalization-group techniques. The system is found to undergo a crossover from a low temperature strongly correlated quantum Hall state to a high-temperature compressible state. This picture is used to account for the recent experimental observation of an anomalous transition in bilayer electron systems [T. S. Lay et al., Phys. Rev. B 50, 17 725 (1994)]. An estimate for the crossover temperature is provided, and it is shown that its dependence on electron density is in reasonable agreement with the experiment.

  • Received 26 October 1999

DOI:https://doi.org/10.1103/PhysRevB.61.4762

©2000 American Physical Society

Authors & Affiliations

M. Abolfath

  • Department of Physics and Astronomy, University of Oklahoma, Norman, Oklahoma 73019-0225
  • Institute for Studies in Theoretical Physics and Mathematics, P.O. Box 19395-5531, Tehran, Iran

Ramin Golestanian

  • Institute for Theoretical Physics, University of California, Santa Barbara, California 93106-4030
  • Institute for Advanced Studies in Basic Sciences, Zanjan 45195-159, Iran

T. Jungwirth

  • Department of Physics, Indiana University, Bloomington, Indiana 47405
  • Institute of Physics ASCR, Cukrovarnická 10, 162 00 Praha 6, Czech Republic

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Vol. 61, Iss. 7 — 15 February 2000

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