Phase diagram of the Kane-Mele-Coulomb model
arXiv:1407.2708 · doi:10.1103/PhysRevB.90.085146
Abstract
We determine the phase diagram of the Kane-Mele model with a long-range Coulomb interaction using an exact quantum Monte Carlo method. Long-range interactions are expected to play a role in honeycomb materials because the vanishing density of states in the semimetallic weak-coupling phase suppresses screening. According to our results, the Kane-Mele-Coulomb model supports the same phases as the Kane-Mele-Hubbard model. The nonlocal part of the interaction promotes short-range sublattice charge fluctuations, which compete with antiferromagnetic order driven by the onsite repulsion. Consequently, the critical interaction for the magnetic transition is significantly larger than for the purely local Hubbard repulsion. Our numerical data are consistent with Gross-Neveu universality for the semimetal to antiferromagnet transition, and with 3D XY universality for the quantum spin Hall to antiferromagnet transition.
9 pages, 7 figures
References in corpus (12)
- The electronic properties of graphene
- Topological Mott Insulators
- Quantum spin-liquid emerging in two-dimensional correlated Dirac fermions
- Interactions and phase transitions on graphene's honeycomb lattice
- Quantum spin Hall effect in a transition metal oxide Na2IrO3
- Absence of a Spin Liquid Phase in the Hubbard Model on the Honeycomb Lattice
- Is graphene in vacuum an insulator?
- Theory of interacting electrons on the honeycomb lattice
- The critical exponents of the superfluid transition in He4
- Correlation effects in two-dimensional topological insulators
- Quantum superconducting criticality in graphene and topological insulators
- Topological Invariant and Quantum Spin Models from Magnetic π Fluxes in Correlated Topological Insulators
Cited by in corpus (13)
- Fermionic quantum criticality in honeycomb and -flux Hubbard models: Finite-size scaling of renormalization-group-invariant observables from quantum Monte Carlo
- Dirac Fermions with Competing Orders: Non-Landau Transition with Emergent Symmetry
- Efficient Continuous-time Quantum Monte Carlo Method for the Ground State of Correlated Fermions
- Temperature and doping induced instabilities of the repulsive Hubbard model on Lieb lattice
- Numerical stabilization of entanglement computation in auxiliary field quantum Monte Carlo simulations of interacting many-fermion systems
- Spontaneous particle-hole symmetry breaking of correlated fermions on the Lieb lattice
- Rashba coupling and magnetic order in correlated helical liquids
- Interplay between the edge-state magnetism and long-range Coulomb interaction in zigzag graphene nanoribbons: quantum Monte Carlo study
- Nature of continuous phase transitions in interacting topological insulators
- Benchmark study of an auxiliary-field quantum Monte Carlo technique for the Hubbard model with shifted-discrete Hubbard-Stratonovich transformations
- Quantum Monte Carlo simulation of topological phase transitions
- Quantum Monte Carlo study of the metal to insulator transition on a honeycomb lattice with 1/r interactions
- Short-ranged interaction effects on topological phase transitions: The perturbative mean-field method