Beyond mean-field behavior of large Bose-Einstein condensates in double-well potentials
arXiv:1308.5805 · doi:10.1103/PhysRevA.88.033608
Abstract
For the dynamics of Bose-Einstein condensates (BECs), differences between mean-field (Gross-Pitaevskii) physics and -particle quantum physics often disappear if the BEC becomes larger and larger. In particular, the timescale for which both dynamics agree should thus become larger if the particle number increases. For BECs in a double-well potential, we find both examples for which this is the case and examples for which differences remain even for huge BECs on experimentally realistic short timescales. By using a combination of numerical and analytical methods, we show that the differences remain visible on the level of expectation values even beyond the largest possible numbers realized experimentally for BECs with ultracold atoms.
10 pages, 4 png figures
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- Chaos in the three-site Bose-Hubbard model -- classical vs quantum
- Stability and Tunneling Dynamics of a Dark-Bright Soliton Pair in a Harmonic Trap
- Negative differential conductivity and quantum statistical effects in a three-site Bose-Hubbard model
- Trojan quasiparticles
- Eigenstate thermalization scaling in approaching the classical limit
- From short-time diffusive to long-time ballistic dynamics: the unusual center-of-mass motion of quantum bright solitons
- The BBGKY hierarchy for ultracold bosonic systems: II. Applications
- Entropy production within a pulsed Bose-Einstein condensate