Abstract
This paper reports a novel type of vortex lattice, referred to as a bubble crystal, which was discovered in rapidly rotating Bose gases with long-range interactions. Bubble crystals differ from vortex lattices which possess a single quantum flux per unit cell, while atoms in bubble crystals are clustered periodically and surrounded by vortices. No existing model is able to describe the vortex structure of bubble crystals; however, we identified a mathematical lattice, which is a subset of coherent states and exists periodically in the physical space. This lattice is called a von Neumann lattice, and when it possesses a single vortex per unit cell, it presents the same geometrical structure as an Abrikosov lattice. In this report, we extend the von Neumann lattice to one with an integral number of flux quanta per unit cell and demonstrate that von Neumann lattices well reproduce the translational properties of bubble crystals. Numerical simulations confirm that, as a generalized vortex, a von Neumann lattice can be physically realized using vortex lattices in rapidly rotating Bose gases with dipole interatomic interactions.
Highlights
Rotating dipolar quantum gases have been shown to contain a number of novel crystal phases[13]
We show that bubble crystals can be approximately represented by vNq lattices with q > 1
We assume that the state of RRDGs is a condensate which is governed by the Gross-Pitaeviskii equation of RRDGs
Summary
Rotating dipolar quantum gases have been shown to contain a number of novel crystal phases[13]. Triangular bubble crystals with an integral number of flux quanta per unit cell are energetically favorable in the regime of a larger blockade radius of RRDGs. We discussed the physical properties of bubble crystals obtained by using the imaginary-time-propagation method to the Gross-Pitaeviskii equation of RRDGs. The case of a vortex lattice with q = 1 corresponds to the Abrikosov lattice, while cases with q > 1 go beyond the Abrikosov model. We extended the von Neumann lattice to one with an integral number of flux quanta per unit cell.
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