Vortices in rotating optical lattices: commensurability, hysteresis, and proximity to the Mott State

Details Vortices in rotating optical lattices: commensurability, hysteresis, and proximity to the Mott State Vortices in rotating optical lattices: commensurability, hysteresis, and proximity to the Mott State

2008-07-23

arxiv.org/abs/0807.3609v1

Physics

Condensed Matter

Other Condensed Matter

21 Pages, 6 Figures ; Higher resolution versions of Figs. 1,4,5 are available upon request

Scientific paper

Quantized vortices stunningly illustrate the coherent nature of a superfluid Bose condensate of alkali atoms. Introducing an optical lattice depletes this coherence. Consequently, novel vortex physics may emerge in an experiment on a harmonically trapped gas in the presence of a rotating optical lattice. The most dramatic effects would occur in proximity to the Mott state, an interaction dominated insulator with a fixed integer number of particles per site. We model such a rotating gas, showing that the lattice-induced spatial profile of the superfluid density drives a gross rearrangement of vortices. For example, instead of the uniform vortex lattices commonly seen in experiments, we find parameters for which the vortices all sit at a fixed distance from the center of the trap, forming a ring. Similarly, they can coalesce at the center, forming a giant vortex. We find that the properties of this system are hysteretic, even far from the Mott state. We explain this hysteresis in terms of vortex pinning, commensurability between vortex density and pinning site density, and energy barriers against changing the number of vortices. Finally, we model time-of-flight expansion, demonstrating the experimental observability of our predictions.

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