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Condensed Fraction of an Atomic Bose Gas Induced by Critical Correlations

Source: Phys. Rev. Lett. 107, 190403 (2011); http://dx.doi.org/10.1103/PhysRevLett.107.190403

Published 2 November 2011

PACS
  • 03.75.Hh
    Static properties of Bose-Einstein condensates
  • 67.85.-d
    Ultracold gases, trapped gases (quantum fluids)
  • YEAR: 2011
PUBLICATION DATA
ISSN:
1935-4061 (online)
Publisher:
AIP is a member of CrossRef APS
Robert P. Smith,1 Naaman Tammuz,1 Robert L. D. Campbell,1 Markus Holzmann,2,3 and Zoran Hadzibabic1
1Cavendish Laboratory, University of Cambridge, J. J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom
2LPTMC, UMR 7600 of CNRS, Université Pierre et Marie Curie, 75752 Paris, France
3LPMMC, UMR 5493 of CNRS, Université Joseph Fourier, 38042 Grenoble, France

We study the condensed fraction of a harmonically trapped atomic Bose gas at the critical point predicted by mean-field theory. The nonzero condensed fraction f0 is induced by critical correlations which increase the transition temperature Tc above T<sub>c</sub><sup>MF</sup>. Unlike the Tc shift in a trapped gas, f0 is sensitive only to the critical behavior in the quasiuniform part of the cloud near the trap center. To leading order in the interaction parameter a/lambda0, where a is the s-wave scattering length and lambda0 the thermal wavelength, we expect a universal scaling f0[proportional](a/lambda0)4. We experimentally verify this scaling using a Feshbach resonance to tune a/lambda0. Further, using the local density approximation, we compare our measurements with the universal result obtained from Monte Carlo simulations for a uniform system, and find excellent quantitative agreement.
History: Received 30 June 2011; published 2 November 2011
Digital Object Identifier: http://dx.doi.org/10.1103/PhysRevLett.107.190403
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