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2016
DOI: 10.1103/physreva.94.053629
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Collective modes of a one-dimensional trapped Bose gas in the presence of the anomalous density

Abstract: We study the collective modes of a one-dimensional (1D) harmonically trapped Bose-Einstein condensate (BEC) in the presence of the anomalous density using the time-dependent-Hartree-FockBogoliubov (TDHFB) theory. Within the hydrodynamic equations, we derive analytical expressions for the mode frequencies and the density fluctuations of the anomalous density which constitutes the minority component at very low temperature and feels an effective external potential exerted by the majority component i.e. the conde… Show more

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Cited by 13 publications
(13 citation statements)
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“…Combining the expressions ofm j andñ j and using the fact that 2N (x) + 1 = coth(x/2), we obtain I kj = coth 2 (ε kj /2T ). For a noninteracting Bose gas where the anomalous density vanishes, I kj = coth 2 (E kj /2T ) [54]. For an ideal trapped case, the Heisenberg invariant keeps the same form as Eq.…”
Section: Tdhfb Theorymentioning
confidence: 93%
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“…Combining the expressions ofm j andñ j and using the fact that 2N (x) + 1 = coth(x/2), we obtain I kj = coth 2 (ε kj /2T ). For a noninteracting Bose gas where the anomalous density vanishes, I kj = coth 2 (E kj /2T ) [54]. For an ideal trapped case, the Heisenberg invariant keeps the same form as Eq.…”
Section: Tdhfb Theorymentioning
confidence: 93%
“…In addition, the TDHFB equations allow us to examine the role of anomalous fluctuations in the phenomenon of phase separation in trapped dual Bose condensates. The anomalous density has a crucial contribution in the stability, excitations, superfluidity, and solitons in a single component BEC [45,46,[54][55][56][57][58][59][60]. Based on experimentally relevant parameters, we demonstrate that a large anomalous density may lead to a transition from miscible to immiscible regime.…”
Section: Introductionmentioning
confidence: 97%
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“…. Expanding the density and the phase in the basis of the excitations: [27,30,36]). Assuming small density fluctuations, we then obtain for the excitation spectrum of homogeneous gas…”
Section: Lhymentioning
confidence: 99%
“…the mean-field energy is repulsive while the beyond mean-field term is attractive [11]. A major advantage of 1D problem which reflected in a supression of three-body losses [12], is that a stable droplet can survive even in strongly-interacting regime due to the boosted role played by quantum fluctuations [13,14]. Difference between bright solitons and quantum droplets have been highlighted in [7,15].…”
Section: Introductionmentioning
confidence: 99%