Rotating Bose gas with hard-core repulsion in a quasi-2D harmonic trap: vortices in BEC
arXiv:cond-mat/0011212 · doi:10.1103/PhysRevA.64.013608
Abstract
We consider a gas of N(=6, 10, 15) Bose particles with hard-core repulsion, contained in a quasi-2D harmonic trap and subjected to an overall angular velocity about the z-axis. Exact diagonalization of the many-body Hamiltonian matrix in given subspaces of the total (quantized) angular momentum L, with (e.g. for L=N=15, n =240782) was carried out using Davidson's algorithm. The many-body variational ground state wavefunction, as also the corresponding energy and the reduced one-particle density-matrix were calculated. With the usual identification of as the Lagrange multiplier associated with L for a rotating system, the phase diagram (or the stability line) was determined that gave a number of critical angular velocities at which the ground state angular momentum and the associated condensate fraction undergo abrupt jumps. A number of (total) angular momentum states were found to be stable at successively higher critical angular velocities for a given N. For , the condensate was strongly depleted. The critical values, however, decreased with increasing interaction strength as well as the particle number, and were systematically greater than the non-variational Yrast-state values for the single vortex state with L =N. We have also observed that the condensate fraction for the single vortex state (as also for the higher vortex states) did not change significantly even as the 2-body interaction strength was varied over several orders of magnitude in the moderately to the weakly interacting regime.
arXiv commentRevtex, 11 pages, 1 table as ps file, 4 figures as ps files
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