Quantum anomalous Hall domains in a Quenched Topological Mott Insulator
arXiv:2502.05035 · doi:10.1103/PhysRevB.111.195141
Abstract
We study an interacting spinless quadratic band touching model that realizes a topological Mott insulating state. We quench the interaction from a value corresponding to the nematic insulator to that of the quantum anomalous Hall (QAH) ordered phase. We perform time-dependent Hartree-Fock simulations and show that after the quench the system realizes an excited Dirac semimetal state, which is however unstable and spontaneously evolves to a state with inhomogeneous nematic and QAH order parameters. The modulations form a stripe pattern that grows exponentially with time until the local Chern marker reaches unity. The alternating QAH order defines a domain structure with boundaries that host chiral sublattice currents.
arXiv comment11 pages, 14 figures
References in corpus (41)
- Quantum Spin Hall Effect in Graphene
- Topological Order and the Quantum Spin Hall Effect
- Ultrafast switching to a stable hidden topologically protected quantum state in an electronic crystal
- Topological Mott Insulators
- Fractional quantum Hall effect in the absence of Landau levels
- Topological Insulators and Nematic Phases from Spontaneous Symmetry Breaking in 2D Fermi Systems with a Quadratic Band Crossing
- Interacting topological insulators: a review
- The simplest quantum model supporting the Kibble-Zurek mechanism of topological defect production: Landau-Zener transitions from a new perspective
- Mapping topological order in coordinate space
- Topological Insulators and Mott Physics from the Hubbard Interaction
- Entanglement Spectrum of a Disordered Topological Chern Insulator
- Spontaneous creation of Kibble-Zurek solitons in a Bose-Einstein condensate
- Quantum Quenches in Chern Insulators
- Interaction effects and quantum phase transitions in topological insulators
- Defect formation beyond Kibble-Zurek mechanism and holography
- Time-Reversal Symmetry Breaking and Spontaneous Anomalous Hall Effect in Fermi Fluids
- From the adiabatic theorem of quantum mechanics to topological states of matter
- Topological Mott Insulator at Quarter Filling in the Interacting Haldane Model
- Mott insulators with boundary zeros
- Transient trapping into metastable states in systems with competing orders
- Low rank compression in the numerical solution of the nonequilibrium Dyson equation
- Global formation of topological defects in the multiferroic hexagonal manganites
- Self-similar dynamics of order parameter fluctuations in pump-probe experiments
- Diagnosis of interaction-driven topological phase via exact diagonalization
- Quenching through Dirac and semi-Dirac points in optical Lattices: Kibble-Zurek scaling for anisotropic Quantum-Critical systems
- Cooper pair turbulence in atomic Fermi gases
- Occupation probabilities and current densities of bulk and edge states of a Floquet topological insulator
- Kibble-Zurek behavior in disordered Chern insulators
- Tunning topological phase and quantum anomalous Hall effect by interaction in quadratic band touching systems
- Adaptive Numerical Solution of Kadanoff-Baym Equations
- Interaction-induced topological phase transition and Majorana edge states in low-dimensional orbital-selective Mott insulators
- Quantum Anomalous Hall Insulator Stabilized By Competing Interactions
- Slow quenches in two-dimensional time-reversal symmetric Z2 topological insulators
- Self-Trapped Polarons and Topological Defects in a Topological Mott Insulator
- Slow quenches in Chern insulator ribbons
- Pattern Formation by Electric-field Quench in Mott Crystal
- Interaction-driven quantum anomalous Hall insulator in Dirac semimetal
- Pattern formation in charge density wave states after a quantum quench
- Ubiquitous nematic Dirac semimetal emerging from interacting quadratic band touching system
- Kibble-Zurek behavior in a topological phase transition with a quadratic band crossing
- Topological phase in the extended Haldane-Hubbard model with sublattice-dependent repulsion