Hamiltonian decomposition for bulk and surface states
arXiv:0811.4000 · doi:10.1103/PhysRevLett.102.146806
Abstract
We demonstrate that a tight-binding Hamiltonian with nearest- and next-nearest-neighbor hopping integrals can be decomposed into bulk and boundary parts in a general lattice system. The Hamiltonian decomposition reveals that next nearest-neighbor hopping causes sizable changes in the energy spectrum of surface states even if the correction to the energy spectrum of bulk states is negligible. By applying the Hamiltonian decomposition to edge states in graphene systems, we show that the next nearest-neighbor hopping stabilizes the edge states.
5 pages, 4 figures
References in corpus (5)
- Stabilization mechanism of edge states in graphene
- Theory of superconductivity of carbon nanotubes and graphene
- Local density of states at zigzag edge of carbon nanotubes and graphene
- Controlling edge states of zigzag carbon nanotubes by the Aharonov-Bohm flux
- Magnetism as a mass term of the edge states in graphene