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DC Field | Value | Language |
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dc.contributor.author | Kaur, P | - |
dc.contributor.author | Gautam, S | - |
dc.contributor.author | Adhikari, S.K | - |
dc.date.accessioned | 2024-06-22T06:13:25Z | - |
dc.date.available | 2024-06-22T06:13:25Z | - |
dc.date.issued | 2024-06-22 | - |
dc.identifier.uri | http://dspace.iitrpr.ac.in:8080/xmlui/handle/123456789/4635 | - |
dc.description.abstract | Abstract We study ultracold superfluid Bose-Fermi mixtures in three dimensions, with stronger confinement along one or two directions, using a non-perturbative beyond-mean-field model for bulk chemical potential valid along the weak-coupling to unitarity crossover. Although bosons are considered to be in a superfluid state, we consider two possibilities for the fermions − spin-polarized degenerate state and superfluid state. Simplified reduced analytic lower-dimensional models are derived along the weak-coupling to unitarity crossover in quasi-one-dimensional (quasi-1D) and quasi-two-dimensional (quasi-2D) settings. The only parameters in these models are the constants of the beyond-mean-field Bose-Bose and Fermi-Fermi Lee-Huang-Yang interactions and the respective universal Bertsch parameter at unitarity. In addition to the numerical results for a fully-trapped system, we also present results for quasi-2D Bose-Fermi mixtures where one of the components is untrapped but localized due to the interaction mediated by the other component. We demonstrate the validity of the reduced quasi-1D and quasi-2D models via a comparison of the numerical solutions for the ground states obtained from the reduced models and the full three-dimensional (3D) model. | en_US |
dc.language.iso | en_US | en_US |
dc.title | Quasi-one- and quasi-two-dimensional Bose-Fermi mixtures from weak coupling to unitarity | en_US |
dc.type | Article | en_US |
Appears in Collections: | Year-2023 |
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