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Quantum phases of tilted dipolar bosons in two-dimensional optical lattice (1906.07483v1)

Published 18 Jun 2019 in cond-mat.quant-gas and physics.atom-ph

Abstract: We consider a minimal model to describe the quantum phases of ultracold dipolar bosons in two-dimensional (2D) square optical lattices. The model is a variation of the extended Bose-Hubbard model and apt to study the quantum phases arising from the variation in the tilt angle $\theta$ of the dipolar bosons. At low tilt angles $0{\circ}\leqslant\theta\apprle25{\circ}$, the ground state of the system are phases with checkerboard order, which could be either checkerboard supersolid or checkerboard density wave. For high tilt angles $55{\circ}\apprge\theta\apprge35{\circ}$, phases with striped order of supersolid or density wave are preferred. In the intermediate domain $25{\circ}\apprle\theta\apprle35{\circ}$ an emulsion or SF phase intervenes the transition between the checkerboard and striped phases. The attractive interaction dominates for $\theta\apprge55{\circ}$, which renders the system unstable and there is a density collapse. For our studies we use Gutzwiller mean-field theory to obtain the quantum phases and the phase boundaries. In addition, we calculate the phase boundaries between an incompressible and a compressible phase of the system by considering second order perturbation analysis of the mean-field theory. The analytical results, where applicable, are in excellent agreement with the numerical results.

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