Interaction driven exotic quantum phases in spin-orbit coupled spin bosons
arXiv:1509.00005 · doi:10.1103/PhysRevB.93.081101
Abstract
We study the interplay between large-spin, spin-orbit coupling, and superfluidity for bosons in a two dimensional optical lattice, focusing on the spin-1 spin-orbit coupled system recently realized at the Joint Quantum Institute [Campbell et. al., arXiv:1501.05984]. We find a rich quantum phase diagram, where, in addition to the conventional phases ---superfluid and insulator--- contained in the spin- Bose-Hubbard model, there are new lattice symmetry breaking phases. For weak interactions, the interplay between two length scales, the lattice momentum and the spin-orbit wave-vector induce a phase transition from a uniform superfluid to a phase where bosons simultaneously condense at the center and edge of the Brillouin zone at a non-zero spin-orbit strength. This state is characterized by spin density wave order, which arises from the spin- nature of the system. Interactions suppress spin density wave order, and favor a superfluid \textit{only} at the Brillouin zone edge. This state has spatially oscillating mean field order parameters, but a homogeneous density. We show that the spin density wave superfluid phase survives in a two dimensional harmonic trap, and thus establish that our results are directly applicable to experiments on Rb, Li, and K.
5 pages, 4 figures, replaced with published version
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- Dynamics of spin-orbit-coupled cold atomic gases in a Floquet lattice with an impurity
- Strongly interacting spin-orbit coupled Bose-Einstein condensates in one dimension
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- Spin-selective Aharonov-Casher caging in a topological quantum network
- Quantum phases of a spin-1 ultracold Bose gas with three body interactions
- Effects of an attractive three body interaction on a spin-1 Bose Hubbard model