Rotating Bose-Einstein condensates: Closing the gap between exact and mean-field solutions
arXiv:1501.05543 · doi:10.1103/PhysRevA.91.033623
Abstract
When a Bose-Einstein condensed cloud of atoms is given some angular momentum, it forms vortices arranged in structures with a discrete rotational symmetry. For these vortex states, the Hilbert space of the exact solution separates into a "primary" space related to the mean-field Gross-Pitaevskii solution and a "complementary" space including the corrections beyond mean-field. Considering a weakly-interacting Bose-Einstein condensate of harmonically-trapped atoms, we demonstrate how this separation can be used to close the conceptual gap between exact solutions for systems with only a few atoms and the thermodynamic limit for which the mean-field is the correct leading-order approximation. Although we illustrate this approach for the case of weak interactions, it is expected to be more generally valid.
8 pages, 5 figures
References in corpus (6)
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- Quantum Hall physics in rotating Bose-Einstein condensates
- Rotating quantum liquids crystallize
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- Rotating Bose-Einstein condensates with a finite number of atoms confined in a ring potential: Spontaneous symmetry breaking, beyond the mean-field approximation
- Dynamics of Ultracold Bosons in Artificial Gauge Fields: Angular Momentum, Fragmentation, and the Variance of Entropy
- Condensates Breaking Up Under Rotation
- Rotation quenches in trapped bosonic systems
- Finite-size effects in the dynamics of few bosons in a ring potential
- Many-body effects in the excitations and dynamics of trapped Bose-Einstein condensates
- A two-state model for vortex nucleation in a rotating Bose-Einstein condensate