paper

Fractional quantum Hall physics with ultracold Rydberg gases in artificial gauge fields

arXiv:1207.3716 · doi:10.1103/PhysRevA.87.043628

Abstract

We study ultracold Rydberg-dressed Bose gases subject to artificial gauge fields in the fractional quantum Hall (FQH) regime. The characteristics of the Rydberg interaction gives rise to interesting many-body ground states different from standard FQH physics in the lowest Landau level (LLL). The non-local but rapidly decreasing interaction potential favors crystalline ground states for very dilute systems. While a simple Wigner crystal becomes energetically favorable compared to the Laughlin liquid for filling fractions , a correlated crystal of composite particles emerges already for with a large energy gap to the simple Wigner crystal. The presence of a new length scale, the Rydberg blockade radius , gives rise to a bubble crystal phase for when the average particle distance becomes less than , which describes the region of saturated, almost constant interaction potential. For larger fillings indications for strongly correlated cluster liquids are found.

9 pages, 10 figures, extended version with additional material

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