Topological delocalization of two-dimensional massless Dirac fermions
The beta function of a two-dimensional massless Dirac Hamiltonian subject to a random scalar potential, which e.g., underlies the theoretical description of graphene, is computed numerically. Although it belongs to, from a symmetry standpoint, the two-dimensional symplectic class, the beta function...
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Published in | arXiv.org |
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Main Authors | , , |
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Language | English |
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17.08.2007
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Abstract | The beta function of a two-dimensional massless Dirac Hamiltonian subject to a random scalar potential, which e.g., underlies the theoretical description 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 \(g\). We also provide an argument based on the spectral flows under twisting boundary conditions, which shows that none of states of the massless Dirac Hamiltonian can be localized. |
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AbstractList | The beta function of a two-dimensional massless Dirac Hamiltonian subject to a random scalar potential, which e.g., underlies the theoretical description 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 \(g\). We also provide an argument based on the spectral flows under twisting boundary conditions, which shows that none of states of the massless Dirac Hamiltonian can be localized. Phys. Rev. Lett. 99, 146806 (2007) The beta function of a two-dimensional massless Dirac Hamiltonian subject to a random scalar potential, which e.g., underlies the theoretical description 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 $g$. We also provide an argument based on the spectral flows under twisting boundary conditions, which shows that none of states of the massless Dirac Hamiltonian can be localized. |
Author | Koshino, Mikito Nomura, Kentaro Ryu, Shinsei |
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BackLink | https://doi.org/10.48550/arXiv.0705.1607$$DView paper in arXiv https://doi.org/10.1103/PhysRevLett.99.146806$$DView published paper (Access to full text may be restricted) |
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DOI | 10.48550/arxiv.0705.1607 |
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Snippet | The beta function of a two-dimensional massless Dirac Hamiltonian subject to a random scalar potential, which e.g., underlies the theoretical description of... Phys. Rev. Lett. 99, 146806 (2007) The beta function of a two-dimensional massless Dirac Hamiltonian subject to a random scalar potential, which e.g.,... |
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SubjectTerms | Boundary conditions Fermions Graphene Physics - Mesoscale and Nanoscale Physics Twisting |
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Title | Topological delocalization of two-dimensional massless Dirac fermions |
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