Edge states and the quantized Hall effect in graphene

Luis Brey and H. A. Fertig
Phys. Rev. B 73, 195408 – Published 10 May 2006

Abstract

We study edges states of graphene ribbons in the quantized Hall regime, and show that they can be described within a continuum model (the Dirac equation) when appropriate boundary conditions are adopted. The two simplest terminations, zigzag and armchair edges, are studied in detail. For zigzag edges, we find that the lowest-Landau-level states terminate in two types of edge states, dispersionless and current-carrying surface states. The latter involve components on different sublattices that may be separated by distances far greater than the magnetic length. For armchair edges, the boundary conditions are met by admixing states from different valleys, and we show that this leads to a single set of edges states for the lowest Landau level and two sets for all higher Landau levels. In both cases, the resulting Hall conductance step for the lowest Landau level is half that between higher Landau levels, as observed in experiment.

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  • Received 21 February 2006

DOI:https://doi.org/10.1103/PhysRevB.73.195408

©2006 American Physical Society

Authors & Affiliations

Luis Brey1 and H. A. Fertig2,1

  • 1Instituto de Ciencia de Materiales de Madrid (CSIC), Cantoblanco, 28049 Madrid, Spain
  • 2Department of Physics, Indiana University, Bloomington, Indiana 47405, USA

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Issue

Vol. 73, Iss. 19 — 15 May 2006

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