First and second sound in a compressible 3D bose fluid

The two-fluid model is fundamental for the description of superfluidity. In the nearly incompressible liquid regime, it successfully describes first and second sound, corresponding, respectively, to density and entropy waves, in both liquid helium and unitary Fermi gases. Here, we study the two soun...

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Asıl Yazarlar: Hilker, TA, Dogra, LH, Eigen, C, Glidden, JAP, Smith, RP, Hadzibabic, Z
Materyal Türü: Journal article
Dil:English
Baskı/Yayın Bilgisi: American Physical Society 2022
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author Hilker, TA
Dogra, LH
Eigen, C
Glidden, JAP
Smith, RP
Hadzibabic, Z
author_facet Hilker, TA
Dogra, LH
Eigen, C
Glidden, JAP
Smith, RP
Hadzibabic, Z
author_sort Hilker, TA
collection OXFORD
description The two-fluid model is fundamental for the description of superfluidity. In the nearly incompressible liquid regime, it successfully describes first and second sound, corresponding, respectively, to density and entropy waves, in both liquid helium and unitary Fermi gases. Here, we study the two sounds in the opposite regime of a highly compressible fluid, using an ultracold <sup>39</sup>K Bose gas in a three-dimensional box trap. We excite the longest-wavelength mode of our homogeneous gas, and observe two distinct resonant oscillations below the critical temperature, of which only one persists above it. In a microscopic mode-structure analysis, we find agreement with the hydrodynamic theory, where first and second sound involve density oscillations dominated by, respectively, thermal and condensed atoms. Varying the interaction strength, we explore the crossover from hydrodynamic to collisionless behavior in a normal gas.
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spelling oxford-uuid:b2d254f6-2bcc-4bbe-a22e-7965e1fa90fb2023-01-04T14:21:11ZFirst and second sound in a compressible 3D bose fluidJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:b2d254f6-2bcc-4bbe-a22e-7965e1fa90fbEnglishSymplectic ElementsAmerican Physical Society2022Hilker, TADogra, LHEigen, CGlidden, JAPSmith, RPHadzibabic, ZThe two-fluid model is fundamental for the description of superfluidity. In the nearly incompressible liquid regime, it successfully describes first and second sound, corresponding, respectively, to density and entropy waves, in both liquid helium and unitary Fermi gases. Here, we study the two sounds in the opposite regime of a highly compressible fluid, using an ultracold <sup>39</sup>K Bose gas in a three-dimensional box trap. We excite the longest-wavelength mode of our homogeneous gas, and observe two distinct resonant oscillations below the critical temperature, of which only one persists above it. In a microscopic mode-structure analysis, we find agreement with the hydrodynamic theory, where first and second sound involve density oscillations dominated by, respectively, thermal and condensed atoms. Varying the interaction strength, we explore the crossover from hydrodynamic to collisionless behavior in a normal gas.
spellingShingle Hilker, TA
Dogra, LH
Eigen, C
Glidden, JAP
Smith, RP
Hadzibabic, Z
First and second sound in a compressible 3D bose fluid
title First and second sound in a compressible 3D bose fluid
title_full First and second sound in a compressible 3D bose fluid
title_fullStr First and second sound in a compressible 3D bose fluid
title_full_unstemmed First and second sound in a compressible 3D bose fluid
title_short First and second sound in a compressible 3D bose fluid
title_sort first and second sound in a compressible 3d bose fluid
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