Interaction-Driven Topological Insulator in Fermionic Cold Atoms on an Optical Lattice: A Design with a Density Functional Formalism
arXiv:1411.3345 · doi:10.1103/PhysRevLett.115.045304
Abstract
We design an interaction-driven topological insulator for fermionic cold atoms in an optical lattice, that is, we pose the question of whether we can realize in a continuous space a spontaneous symmetry breaking induced by the inter-atom interaction into a topological Chern insulator. Such a state, sometimes called a "topological Mott insulator", has yet to be realized in solid-state systems, since this requires, in the tight-binding model, large offsite interactions on top of a small onsite interaction. Here we overcome the difficulty by introducing a spin-dependent potential, where a spin-selective occupation of fermions in and sublattices makes the onsite interaction Pauli-forbidden, while a sizeable inter-site interaction is achieved by a shallow optical potential with a large overlap between neighboring Wannier orbitals. This puts the system away from the tight-binding model, so that we adopt the density functional theory for cold-atoms, here extended to accommodate non-collinear spin structures emerging in the topological regime, to quantitatively demonstrate the phase transition to the topological Mott insulator.
5+8 pages, 3+3 figures
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Cited by in corpus (7)
- Interaction-Driven Spontaneous Quantum Hall Effect on Kagome Lattice
- Quantum Simulation of a Topological Mott Insulator with Rydberg Atoms in a Lieb Lattice
- Diagnosis of interaction-driven topological phase via exact diagonalization
- Tunning topological phase and quantum anomalous Hall effect by interaction in quadratic band touching systems
- Quantum Anomalous Hall Insulator Stabilized By Competing Interactions
- Stabilization of Topological Insulator Emerging from Electron Correlations on Honeycomb Lattice and Its Possible Relevance in Twisted Bilayer Graphene
- Chern Kondo Insulator in an Optical Lattice