Coupling, merging, and splitting Dirac points by electron-electron interaction
arXiv:1305.7320 · doi:10.1103/PhysRevB.88.075126
Abstract
The manipulation and movement of Dirac points in the Brillouin zone by the electron-electron interaction is considered within leading order perturbation theory. At the merging point, an infinitesimal interaction is shown to cause opening of the gap or splitting of the Dirac points, depending on the inter- or intrasublattice nature of the merging and the sign of the interaction. The topology of the spectrum can therefore be efficiently changed by simply tuning the interaction between particles, as opposed to the usual careful band structure engineering. This is illustrated around the merging transition of one, two, and three dimensional Dirac-Weyl fermions. A simple Weyl-like Hamiltonian that describes the quadratic band-crossing in three dimensions is also proposed, and its stability under interactions is addressed.
6 pages, 3 figures, published version
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- Nematic, topological and Berry phases when a flat and a parabolic band touch
- Quantum phase transitions in Dirac fermion systems
- Excitonic pairing and insulating transition in two-dimensional semi-Dirac semimetals
- Semi-Dirac Fermions in a Topological Metal
- Non-monotonic response and light-cone freezing in gapless-to-(partially) gapped quantum quenches of fermionic systems
- Interplay of Coulomb interaction and disorder in a two-dimensional semi-Dirac fermion system
- Coulomb interactions and renormalization of semi-Dirac fermions near a topological Lifshitz transition
- Quantum Monte Carlo simulation of topological phase transitions
- Microscopic lattice model for quartic semi-Dirac fermions in two dimensions
- Fate of superconductivity in disordered Dirac and semi-Dirac semimetals
- Dirac points merging and wandering in a model Chern insulator
- Semi-Dirac spin liquids and frustrated quantum magnetism on the trellis lattice
- Anomaly non-renormalization in interacting Weyl semimetals