Finite-momentum Bose-Einstein condensates in shaken 2D square optical lattices
arXiv:1104.4350 · doi:10.1103/PhysRevA.84.013607
Abstract
We consider ultracold bosons in a 2D square optical lattice described by the Bose-Hubbard model. In addition, an external time-dependent sinusoidal force is applied to the system, which shakes the lattice along one of the diagonals. The effect of the shaking is to renormalize the nearest-neighbor hopping coefficients, which can be arbitrarily reduced, can vanish, or can even change sign, depending on the shaking parameter. It is therefore necessary to account for higher-order hopping terms, which are renormalized differently by the shaking, and introduce anisotropy into the problem. We show that the competition between these different hopping terms leads to finite-momentum condensates, with a momentum that may be tuned via the strength of the shaking. We calculate the boundaries between the Mott-insulator and the different superfluid phases, and present the time-of-flight images expected to be observed experimentally. Our results open up new possibilities for the realization of bosonic analogs of the FFLO phase describing inhomogeneous superconductivity.
7 pages, 7 figures
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- Quantum Phase Transition of Bosons in a Shaken Optical Lattice
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- Fast and direct preparation of a genuine lattice BEC via the quantum Mpemba effect
- Extended Bose-Hubbard model in a shaken optical lattice
- Symmetry-protected Bose-Einstein condensation of interacting hardcore Bosons