We investigate thermal relaxation of superfluid turbulence in a highly oblate Bose-Einstein condensate. We generate turbulent flow in the condensate by sweeping the center region of the condensate with a repulsive optical potential. The turbulent condensate shows a spatially disordered distribution of quantized vortices, and the vortex number of the condensate exhibits nonexponential decay behavior which we attribute to the vortex pair annihilation. The vortex-antivortex collisions in the condensate are identified with crescent-shaped, coalesced vortex cores. We observe that the nonexponential decay of the vortex number is quantitatively well described by a rate equation consisting of one-body and two-body decay terms. In our measurement, we find that the local two-body decay rate is closely proportional to T2/μ, where T is the temperature and μ is the chemical potential.
Relaxation of superfluid turbulence in highly oblate Bose-Einstein condensates / W.J. Kwon, G. Moon, J. Choi, S. Won Seo, Y. Shin. - In: PHYSICAL REVIEW A. - ISSN 1050-2947. - 90:6(2014 Dec 19), pp. 063627.1-063627.6. [10.1103/physreva.90.063627]
Relaxation of superfluid turbulence in highly oblate Bose-Einstein condensates
W.J. KwonPrimo
;
2014
Abstract
We investigate thermal relaxation of superfluid turbulence in a highly oblate Bose-Einstein condensate. We generate turbulent flow in the condensate by sweeping the center region of the condensate with a repulsive optical potential. The turbulent condensate shows a spatially disordered distribution of quantized vortices, and the vortex number of the condensate exhibits nonexponential decay behavior which we attribute to the vortex pair annihilation. The vortex-antivortex collisions in the condensate are identified with crescent-shaped, coalesced vortex cores. We observe that the nonexponential decay of the vortex number is quantitatively well described by a rate equation consisting of one-body and two-body decay terms. In our measurement, we find that the local two-body decay rate is closely proportional to T2/μ, where T is the temperature and μ is the chemical potential.| File | Dimensione | Formato | |
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