2010
DOI: 10.1016/j.physa.2009.12.017
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Thermodynamics of Bose–Einstein gas trapped in -dimensional quartic potentials

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Cited by 17 publications
(10 citation statements)
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“…The shift in the condensation temperature respect to the ideal result, caused by the interactions among the constituents of the gas is about 5 × 10 −2 with a 1% of error [31]. For instance, under typical conditions the number of particles is about N ∼ 10 6 − 10 5 in three dimensions [34]; for one dimensional systems, the number of particles can be estimated up to N ∼ 10 4 [52,54,55]. Using typical frequencies of order 100 Hz, allows us to bound the polymer scale up to λ 2 10 −16 m 2 , which is notable.…”
Section: Condensation Temperaturementioning
confidence: 99%
“…The shift in the condensation temperature respect to the ideal result, caused by the interactions among the constituents of the gas is about 5 × 10 −2 with a 1% of error [31]. For instance, under typical conditions the number of particles is about N ∼ 10 6 − 10 5 in three dimensions [34]; for one dimensional systems, the number of particles can be estimated up to N ∼ 10 4 [52,54,55]. Using typical frequencies of order 100 Hz, allows us to bound the polymer scale up to λ 2 10 −16 m 2 , which is notable.…”
Section: Condensation Temperaturementioning
confidence: 99%
“…The presence of the interactions also affects the relative behaviour of the condensate fractions in both traps. As opposed to the non-interacting case, which has been recently studied by Karabulut et al [11], it is seen in this case that the condensation in the quartic trap exhibits a sharper increase with temperature (inset, Fig. 2).…”
Section: Resultsmentioning
confidence: 56%
“…As the strength of interactions is increased the peak-like structure of specific heat, which pertains to systems with finite particle number (see Ref. [11]), is deformed gradually. It is also seen from the figure that, for η = 0.05, the specific heat is almost zero at a temperature very close to T 0 .…”
Section: Resultsmentioning
confidence: 99%
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