2012
DOI: 10.1088/0031-8949/86/05/055001
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Shortcuts to adiabaticity for growing condensates

Abstract: We investigate fast frictionless expansion for growing Bose–Einstein condensates described by the Gross–Pitaevskii gain equation. We show that fast frictionless expansion can be generalized to a condensate continuously replenished by pumping from the reservoir. We apply our formalism to the harmonically trapped condensate and an optical lattice.

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Cited by 5 publications
(5 citation statements)
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“…Decreasing the potential depth as V (t) = V 0 /Λ 2 (t), and making the first and second derivatives of Λ vanish at the boundary times guarantee a frictionless expansion. In Ozcakmakli and Yuce (2012) the results are extended to a continuously replenished BEC in a harmonic trap or in an optical lattice. Lau and James (2012) propose inverse engineering of the trap frequencies based on the Lewis-Riesenfeld invariants as part of the elementary operations necessary to implement a universal bosonic simulator using ions in separate traps.…”
Section: Other Applicationsmentioning
confidence: 99%
See 1 more Smart Citation
“…Decreasing the potential depth as V (t) = V 0 /Λ 2 (t), and making the first and second derivatives of Λ vanish at the boundary times guarantee a frictionless expansion. In Ozcakmakli and Yuce (2012) the results are extended to a continuously replenished BEC in a harmonic trap or in an optical lattice. Lau and James (2012) propose inverse engineering of the trap frequencies based on the Lewis-Riesenfeld invariants as part of the elementary operations necessary to implement a universal bosonic simulator using ions in separate traps.…”
Section: Other Applicationsmentioning
confidence: 99%
“…1 There the Lewis-Riesenfeld invariants were used to inverse engineer the time dependence of a harmonic oscillator frequency between predetermined initial and final values so as to avoid final excitations. That paper and its companion on Bose-Einstein condensates (Muga et al, 2009) have indeed triggered a surge of activity, not only for harmonic expansions (Chen and Muga, 2010;Muga et al, 2010;Stefanatos et al, 2010;Schaff et al, 2010Schaff et al, , 2011adel Campo, 2011a;Schaff et al, 2011b;Stefanatos et al, 2011;Torrontegui et al, 2012c;Fasihi et al, 2012;Torrontegui et al, 2012a;del Campo and Boshier, 2012;Stefanatos and Li, 2012), but for atom transport (Torrontegui et al, 2011(Torrontegui et al, , 2012dChen et al, 2011b;Bowler et al, 2012), quantum computing (Sarandy et al, 2011), quantum simulations (Lau and James, 2012), optical lattice expansions (Yuce, 2012;Ozcakmakli and Yuce, 2012), wavepacket splitting (Torrontegui et al, 2012b), internal state control (Chen et al, 2011a;Ibáñez et al, 2011;Ruschhaupt et al, 2012;Ban et al, 2012;Ibáñez et al, 2012a;Güngördü et al, 2012), many-body state engineering (del Campo, 2011b;del Campo and Boshier, 2012;Juliá-Díaz et al, 2012), and other applications such as sympathetic cooling of atomic mixtures (Choi, Onofrio and Sundaram, 2011;Choi et al, 2012), or cooling of nanomechanical resonators ...…”
mentioning
confidence: 96%
“…We close this section by mentioning that other non-linear processes that can be assisted by CD include the (meanfield) growth dynamics of a Bose-Einstein condensate [69]. Nonetheless, phase fluctuations in the newborn condensate are expected to result in the formation of solitons [70] or vortices [71], depending in the dimensionality, as dictated by the Kibble-Zurek mechanism [72,73].…”
Section: Counderdiabatic Driving Of Nonlinear Systemsmentioning
confidence: 99%
“…The chemical potential μ is determined via the normalization condition. Considering the TF limit in the scaling GPE (6) and choosing scaling functions as [35] a…”
Section: A Interaction Rampmentioning
confidence: 99%
“…Considering the TF limit in the scaling GPE Eq. ( 6) and choosing scaling functions as [35] ä + ω 2 a = ω 2 g(t) gi…”
Section: A Interaction Rampmentioning
confidence: 99%