Open AccessFermionization and fractional statistics in the strongly interacting one‐dimensional Bose gas
Author(s) -
Batchelor M. T.,
Guan X.W.
Publication year - 2007
Publication title -
laser physics letters
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.59
H-Index - 72
eISSN - 1612-202X
pISSN - 1612-2011
DOI - 10.1002/lapl.200610068
Subject(s) - bose gas , physics , boson , statistics , quantum statistical mechanics , fermi gamma ray space telescope , measure (data warehouse) , ideal gas , distribution (mathematics) , fermi gas , equivalence (formal languages) , quantum mechanics , statistical physics , quantum , bose–einstein condensate , mathematical analysis , mathematics , discrete mathematics , database , computer science , electron
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 87 Rb 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)