Graphene with geometrically induced vorticity
arXiv:0710.0858 · doi:10.1103/PhysRevLett.100.156806
Abstract
At half filling, the electronic structure of graphene can be modelled by a pair of free two-dimensional Dirac fermions. We explicitly demonstrate that in the presence of a geometrically induced gauge field, an everywhere-real Kekule modulation of the hopping matrix elements can correspond to a non-real Higgs field with non-trivial vorticity. This provides a natural setting for fractionally charged vortices with localized zero modes. For fullerene-like molecules we employ the index theorem to demonstrate the existence of six low-lying states that do not depend strongly on the Kekule-induced mass gap.
4 pages, 3 figures, to appear in PRL
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- Weyl-Gauge Symmetry of Graphene
- Manifestations of topological effects in graphene
- Probing non-Hermitian phase transitions in curved space via quench dynamics
- Yang-Mills gauge theories from fermionic lattice models
- Topological gap states of semiconducting armchair graphene ribbons
- Fullerenes, Zero-modes, and Self-adjoint Extensions
- Conductance enhancement due to atomic potential fluctuations in graphene
- Effect of topological defects and Coulomb charge on the low energy quantum dynamics of gapped graphene
- Majorana zero modes in graphene with trigonal warping
- Induced fractional valley number in graphene with topological defects
- Quantum geometric tensors from sub-bundle geometry
- Topological Vortices in Chiral Gauge Theory of Graphene
- On topological aspects of 2D graphene like materials
- Fermionic zero modes in the vortex field in arbitrary dimensions and index of Dirac operator with Majorana-like interaction
- On geometric delusions of hexagonal structures