Merging Dirac points and topological phase transitions in the tight-binding model on the generalized honeycomb lattice
arXiv:1207.6841 · doi:10.1103/PhysRevB.86.165430
Abstract
Moving, merging and annihilating Dirac points are studied theoretically in the tight-binding model on honeycomb lattice with up-to third-nearest-neighbor hoppings. We obtain a rich phase diagram of the topological phase transitions in the parameter space of direction-dependent hoppings. We obtain the conditions for the three Dirac points to merge and for the tricritical points. We find that only very small third-nearest-neighbor hoppings are enough for the existence of the merging of three-Dirac-points and the tricritical points, if the system is sufficiently anisotropic. The density of states is obtained to be when three Dirac points merge, and at the tricritical points. It is possible to realize these topological phase transitions in the ultracold atoms on the optical lattice, strained monolayer graphene or strained bilayer graphene.
19 pages, 25 figures
References in corpus (12)
- Electric Field Effect in Atomically Thin Carbon Films
- Substrate-induced band gap opening in epitaxial graphene
- A tight-binding approach to uniaxial strain in graphene
- Quantum transport of massless Dirac fermions in graphene
- Merging of Dirac points in a two-dimensional crystal
- Gap opening in graphene by shear strain
- A new magnetic field dependence of Landau levels on a graphene like structure
- Zero modes of tight binding electrons on the honeycomb lattice
- Comment on "Band structure engineering of graphene by strain: First-principles calculations"
- Effects of the Zero-Mode Landau Level on Inter-Layer Magnetoresistance in Multilayer Massless Dirac Fermion Systems
- Topologically Protected Zero Modes in Twisted Bilayer Graphene
- Strained bilayer graphene: Band structure topology and Landau level spectrum