Abstract:We analyse numerically the finite-temperature behaviour of a dilute trapped Bose gas containing a large number of atoms. The generalized Hartree-Fock-Bogoliubov approximation is used to take into account the mutual interactions between the condensate and the thermal cloud. We confront our results with recent experiments and literature and explain in particular the experimentally observed departure from the Thomas-Fermi regime for the condensate radius and the aspect ratio. This clearly illustrates the compress… Show more
“…The equation (2.7) involves an explicitly diverging term (for r = r ′ ) which should be regularized. To this end, one may absorb this diverging expression in a redefinition of the thermal average [7,8,19] or, as performed by [20,21], one may use the pseudopotential method [22] to renormalize the coupling constant. A more rigorous approach is the Λ-potential method first discussed in [9,10].…”
We study the anomalous density in an ultra-cold trapped bose gas in a variational framework, for both zero and finite temperature. We show that it is finite in 1D, while it is logarithmically and linearly divergent in 2D and 3D. The renormalization that we adopt is more reliable and compatible with the variational scheme. The main outcome is that the anomalous and non condensate densities are of the same order of magnitude and should therefore be treated on an equal footing.
“…The equation (2.7) involves an explicitly diverging term (for r = r ′ ) which should be regularized. To this end, one may absorb this diverging expression in a redefinition of the thermal average [7,8,19] or, as performed by [20,21], one may use the pseudopotential method [22] to renormalize the coupling constant. A more rigorous approach is the Λ-potential method first discussed in [9,10].…”
We study the anomalous density in an ultra-cold trapped bose gas in a variational framework, for both zero and finite temperature. We show that it is finite in 1D, while it is logarithmically and linearly divergent in 2D and 3D. The renormalization that we adopt is more reliable and compatible with the variational scheme. The main outcome is that the anomalous and non condensate densities are of the same order of magnitude and should therefore be treated on an equal footing.
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