Topological aspect of graphene physics
arXiv:1008.4653 · doi:10.1088/1742-6596/334/1/012004
Abstract
Topological aspects of graphene are reviewed focusing on the massless Dirac fermions with/without magnetic field. Doubled Dirac cones of graphene are topologically protected by the chiral symmetry. The quantum Hall effect of the graphene is described by the Berry connection of a manybody state by the filled Landau levels which naturally possesses non-Abelian gauge structures. A generic principle of the topologically non trivial states as the bulk-edge correspondence is applied for graphene with/without magnetic field and explain some of the characteristic boundary phenomena of graphene.
12 pages, 8 figures. Proceedings for HMF-19
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Cited by in corpus (17)
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- The Rare Two-Dimensional Materials with Dirac Cones
- Nonlinear quantum optical properties of graphene: the role of chirality and symmetry
- Antichiral states in twisted graphene multilayers
- Quantum criticality in the metal-superconductor transition of interacting Dirac fermions on a triangular lattice
- Landau Levels in Uniaxially Strained Graphene: A Geometrical Approach
- SU(3) Dirac electrons in the 1/5-depleted square-lattice Hubbard model at 1/4 filling
- Survival of sharp Landau levels in massive tilted Dirac fermions: Protection by generalized chiral operator
- Bulk-edge correspondence with generalized chiral symmetry
- Topologically protected Landau levels in bilayer graphene in finite electric fields
- Dirac fermions in graphene and analogues: magnetic field and topological properties
- Pseudo chiral anomaly in zigzag graphene ribbons
- Topologically Protected Doubling of Tilted Dirac Fermions in Two Dimensions
- Fermi point in graphene as a monopole in momentum space
- Green functions in graphene monolayer with Coulomb interactions taken into account
- On topological aspects of 2D graphene like materials
- Chiral Symmetry and Many-Body Effect in Multilayer Graphene