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Topological Delocalization of Two-Dimensional Massless Dirac Fermions

2007/05/31 by Kentaro Nomura, Mikito Koshino, Shinsei Ryu · 8 citations
Materials Science · Physics and Astronomy · #Graphene research and applications #Noncommutative and Quantum Gravity Theories #Topological Materials and Phenomena #cond-mat.mes-hall

paper · pdf · doi:10.1103/physrevlett.99.146806

published as Phys. Rev. Lett. 99, 146806 (2007) · 4 pages, 2 figures

arxiv created 2007/08/17 · openalex publication_date 2007/10/05 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28

Abstract

The beta function of a two-dimensional massless Dirac Hamiltonian subject to a random scalar potential, which, e.g., underlies theoretical descriptions of graphene, is computed numerically. Although it belongs to, from a symmetry standpoint, the two-dimensional symplectic class, the beta function monotonically increases with decreasing conductance. We also provide an argument based on the spectral flows under twisting boundary conditions, which shows that none of the states of the massless Dirac Hamiltonian can be localized.

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