Microscopic Realization of 2-Dimensional Bosonic Topological Insulators
arXiv:1404.2818 · doi:10.1103/PhysRevLett.113.267206
Abstract
It is well known that a Bosonic Mott insulator can be realized by condensing vortices of a bo- son condensate. Usually, a vortex becomes an anti-vortex (and vice-versa) under time reversal symmetry, and the condensation of vortices results in a trivial Mott insulator. However, if each vortex or anti-vortex interacts with a spin trapped at its core, the time reversal transformation of the composite vortex operator will contain an extra minus sign. It turns out that such a composite vortex condensed state is a bosonic topological insulator (BTI) with gapless boundary excitations protected by symmetry. We point out that in BTI, an external flux monodromy defect carries a Kramers doublet. We propose lattice model Hamiltonians to realize the BTI phase, which might be implemented in cold atom systems or spin-1 solid state systems.
5 pages + supplementary material
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Cited by in corpus (10)
- Chiral Mott Insulators, Meissner Effect, and Laughlin States in Quantum Ladders
- Construction of bosonic symmetry-protected-trivial states and their topological invariants via non-linear -models
- Vortex-line condensation in three dimensions: A physical mechanism for bosonic topological insulators
- Chiral Bosonic Phases on the Haldane Honeycomb Lattice
- Symmetry-protected Topological Phases at Finite Temperature
- Symmetry Enrichment in Three-Dimensional Topological Phases
- Simulating bosonic Chern insulators in one-dimensional optical superlattices
- Hidden order and flux attachment in symmetry protected topological phases: a Laughlin-like approach
- Fermionic Symmetry Protected Topological Phase Induced by Interactions
- Solvable lattice model for (2+1)D bosonic topological insulator