2021
DOI: 10.48550/arxiv.2103.15283
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On the survival of the quantum depletion of a condensate after release from a magnetic trap

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Cited by 5 publications
(8 citation statements)
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References 78 publications
(145 reference statements)
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“…This formed a sensitive measurement of the optical dipole polarizability of helium and in turn the tune-out frequency, at which the dipole polarizability vanishes, as a stringent test of QED. The ability to measure the trap frequency of multiple axes simultaneously allowed for quick calibration in [8] where it was used to quantitatively compare theoretical predictions with experimental measurements. In [38] we used both the frequency and amplitude and measurements as a measure of excitation after superfluid transport.…”
Section: Discussionmentioning
confidence: 99%
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“…This formed a sensitive measurement of the optical dipole polarizability of helium and in turn the tune-out frequency, at which the dipole polarizability vanishes, as a stringent test of QED. The ability to measure the trap frequency of multiple axes simultaneously allowed for quick calibration in [8] where it was used to quantitatively compare theoretical predictions with experimental measurements. In [38] we used both the frequency and amplitude and measurements as a measure of excitation after superfluid transport.…”
Section: Discussionmentioning
confidence: 99%
“…Improving the precision, speed and convenience of trap frequency measurement will allow higher precision investigations of BEC physics including many body physics phenomena (e.g. quantum depletion [7][8][9], thermalization [10], collective excitations [11], and phase transitions [12]) and improve the capability of curvature sensing.…”
Section: Introductionmentioning
confidence: 99%
“…[45] (see also [50]). Such equations have been used to successfully describe several experimental results on Bose-Einstein condensate collisions [45,[51][52][53][54][55][56], and a more recent extension of this approach was used to characterize the quantum depletion of an expanding condensate [57]. We point out that the stochastic Bogoliubov equations themselves are equivalent to the usual Bogoliubov approach [15,16,58,59] in which the Bose field operator is expanded as Ψ = Ψ 0 + δ ψ where Ψ 0 is the mean-field order parameter obeying equation ( 22) and δ ψ represents small fluctuations around the mean-field obeying…”
Section: Comparison With Bogoliubov Approachesmentioning
confidence: 99%
“…Some situations where this type of advantage has already been exploited can be found in Refs. [45,55,57]. In these cases, the systems being considered require an extremely large numerical lattice or an unreasonable number of modes for simulation.…”
Section: Comparison With Bogoliubov Approachesmentioning
confidence: 99%
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