Fermionization and fractional statistics in the strongly interacting one-dimensional Bose gas

We discuss recent results on the relation between the strongly interacting one‐dimensional Bose gas and a gas of ideal particles obeying nonmutual generalized exclusion statistics (GES). The thermodynamic properties considered include the statistical profiles, the specific heat and local pair correl...

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Published inLaser physics letters Vol. 4; no. 1; pp. 77 - 83
Main Authors Batchelor, M. T., Guan, X.-W.
Format Journal Article
LanguageEnglish
Published Berlin WILEY-VCH Verlag 01.01.2007
WILEY‐VCH Verlag
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Summary:We discuss recent results on the relation between the strongly interacting one‐dimensional Bose gas and a gas of ideal particles obeying nonmutual generalized exclusion statistics (GES). The thermodynamic properties considered include the statistical profiles, the specific heat and local pair correlations. In the strong coupling limit γ → ∞, the Tonks‐Girardeau gas, the equivalence is with Fermi statistics. The deviation from Fermi statistics during boson fermionization for finite but large interaction strength γ is described by the relation α ≈ 1 – 2/γ, where α is a measure of the GES. This gives a quantitative description of the fermionization process. In this sense the recent experimental measurement of local pair correlations in a 1D Bose gas of 87Rb atoms also provides a measure of the deviation of the GES parameter α away from the pure Fermi statistics value α = 1. Other thermodynamic properties, such as the distribution profiles and the specific heat, are also sensitive to the statistics. They also thus provide a way of exploring fractional statistics in the strongly interacting 1D Bose gas. (© 2006 by Astro, Ltd. Published exclusively by WILEY‐VCH Verlag GmbH & Co. KGaA)
Bibliography:ArticleID:LAPL200610068
istex:170D7B7D5447F583CD902B04CC5EF8AEBBA397C5
ark:/67375/WNG-SK8XRPST-M
Australian Research Council
ISSN:1612-2011
1612-202X
DOI:10.1002/lapl.200610068