2003
DOI: 10.1103/physreva.67.013605
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Controlling collapse in Bose-Einstein condensates by temporal modulation of the scattering length

Abstract: We consider, by means of the variational approximation ͑VA͒ and direct numerical simulations of the Gross-Pitaevskii ͑GP͒ equation, the dynamics of two-dimensional ͑2D͒ and 3D condensates with a scattering length containing constant and harmonically varying parts, which can be achieved with an ac magnetic field tuned to the Feshbach resonance. For a rapid time modulation, we develop an approach based on the direct averaging of the GP equation, without using the VA. In the 2D case, both VA and direct simulation… Show more

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Cited by 346 publications
(175 citation statements)
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“…Thus the inclusion of three-body interaction seems to increase the stability of the condensates. The stability of trapless BEC with two-body interaction for constant (slowly varying) and oscillatory (rapidly varying) part has been already explored [28,32,33]. However, to the best of our knowledge, the effect on the inclusion of three-body interaction has not been studied in trapless BEC.…”
Section: Variational Approximationmentioning
confidence: 99%
“…Thus the inclusion of three-body interaction seems to increase the stability of the condensates. The stability of trapless BEC with two-body interaction for constant (slowly varying) and oscillatory (rapidly varying) part has been already explored [28,32,33]. However, to the best of our knowledge, the effect on the inclusion of three-body interaction has not been studied in trapless BEC.…”
Section: Variational Approximationmentioning
confidence: 99%
“…In Bose-Einstein conden-sates it is experimentally feasible to vary the scattering length by either magnetically or optically inducing a Feshbach resonance [4,14]. Earlier works on Bose-Einstein condensation report the periodic modulation with constant frequency of scattering length [5,7,8,9]. Along these lines, it is of potential interest to understand the dynamics of Bose-Einstein condensates under the action of periodically varying scattering length with slowly varying frequency.…”
Section: Introductionmentioning
confidence: 99%
“…According to the variational method we assume the Gaussian wave function in the form [7,8,9,19,20,21] φ(r, t) = A(t) exp − r 2 2a(t) 2 + ib(t) 2 r 2 2 + iδ(t) ,…”
Section: Variational Proceduresmentioning
confidence: 99%
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