Joule-Thomson coefficient of ideal anyons within fractional exclusion statistics
arXiv:1101.4436 · doi:10.1103/PhysRevE.83.021111
Abstract
The analytical expressions of the Joule-Thomson coefficient for homogeneous and harmonically trapped three-dimensional ideal anyons which obey Haldane fractional exclusion statistics are derived. For an ideal Fermi gas, the Joule-Thomson coefficient is negative, which means that there is no maximum Joule-Thomson inversion temperature. With careful study, it is found that there exists a Joule-Thomson inversion temperature in the fractional exclusion statistics model. Furthermore, the relations between the Joule-Thomson inversion temperature and the statistical parameter are investigated.
arXiv comment6 pages, 3 figures, minor changes with typos corrected
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- Equivalence between fractional exclusion statistics and self-consistent mean-field theory in interacting particle systems in any number of dimensions
- From Fractional Exclusion Statistics Back to Bose and Fermi Distributions