Zero modes and the edge states of the honeycomb lattice
arXiv:cond-mat/0702162 · doi:10.1103/PhysRevB.76.205402
Abstract
The honeycomb lattice in the cylinder geometry with zigzag edges, bearded edges, zigzag and bearded edges (zigzag-bearded), and armchair edges are studied. The tight-binding model with nearest-neighbor hoppings is used. Edge states are obtained analytically for these edges except the armchair edges. It is shown, however, that edge states for the armchair edges exist when the the system is anisotropic. These states have not been known previously. We also find strictly localized states, uniformly extended states and states with macroscopic degeneracy.
6 pages 8 figures
References in corpus (8)
- Energy Gaps in Graphene Nanoribbons
- Half-Metallic Graphene Nanoribbons
- Electronic States of Graphene Nanoribbons
- Peculiar Width Dependence of the Electronic Property of Carbon Nanoribbons
- Spin Filtered Edge States and Quantum Hall Effect in Graphene
- Zero modes of tight binding electrons on the honeycomb lattice
- Gauge field for edge state in graphene
- Quantum Hall effect and the topological number in graphene
Cited by in corpus (6)
- Spectrum of -electrons in Graphene As a Macromolecule
- Spectrum of Electrons in Graphene as an Alternant Macromolecule and Its Specific Features in Quantum Conductance
- Zero modes, energy gap, and edge states of anisotropic honeycomb lattice in a magnetic field
- Edge states of zigzag bilayer graphite nanoribbons
- Quantum Phase Transition in Hall Conductivity on an Anisotropic Kagome Lattice
- Edge states in the three-quarter filled system, -(BEDT-TTF)I