Quantum Hall Effect of Massless Dirac Fermions in a Vanishing Magnetic Field

Kentaro Nomura, Shinsei Ryu, Mikito Koshino, Christopher Mudry, and Akira Furusaki
Phys. Rev. Lett. 100, 246806 – Published 20 June 2008

Abstract

The effect of strong long-range disorder on the quantization of the Hall conductivity σxy in graphene is studied numerically. It is shown that increasing Landau-level mixing progressively destroys all plateaus in σxy except the plateaus at σxy=e2/2h (per valley and per spin). The critical state at the Dirac point is robust to strong disorder and belongs to the universality class of the conventional plateau transitions in the integer quantum Hall effect. We propose that the breaking of time-reversal symmetry by ripples in graphene can realize this quantum critical point in a vanishing magnetic field.

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  • Received 20 January 2008

DOI:https://doi.org/10.1103/PhysRevLett.100.246806

©2008 American Physical Society

Authors & Affiliations

Kentaro Nomura1, Shinsei Ryu2, Mikito Koshino3,4, Christopher Mudry5, and Akira Furusaki6

  • 1Department of Physics, Tohoku University, Sendai, 980-8578, Japan
  • 2Kavli Institute for Theoretical Physics, University of California, Santa Barbara, California 93106, USA
  • 3Department of Physics, Tokyo Institute of Technology, Meguro-ku, Tokyo 152-8551, Japan
  • 4Physics Department, Columbia University, New York, New York 10027, USA
  • 5Condensed Matter Theory Group, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
  • 6Condensed Matter Theory Laboratory, RIKEN, Wako, Saitama 351-0198, Japan

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Issue

Vol. 100, Iss. 24 — 20 June 2008

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