Comment on ``Quantum Statistical Mechanics of an Ideal Gas with Fractional Exclusion Statistics in Arbitrary Dimension"

dc.creatorHuang, Wung-Hong
dc.date2007-02-05
dc.date.accessioned2026-07-07T11:40:43Z
dc.date.available2026-07-07T11:40:43Z
dc.descriptionIt is mentioned that anyon thermodynamic potential $Q(α, N)$ could not be factorized in terms characteristic of the ideal boson $α=0$ and fermion $α=1$ gases by the relation $Q(α, N) = (1-α) Q(0, N_b)+ αQ(1, N_f)$ in which $N=N_f +N_b$, that claimed in Phys. Rev. Lett. 78, 3233 (1997). Our analyses indicate that the thermodynamic quantities of anyon gas may be factorized as $Q(α) = αQ(1) + (1-α) Q(0)$ only in the two-dimension system.
dc.identifierhttps://arxiv.org/abs/cond-mat/0702075
dc.identifierhttp://arxiv.org/abs/cond-mat/0702075
dc.identifierPhys.Rev.Lett.81:2392,1998
dc.identifierdoi:10.1103/PhysRevLett.81.2392
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/200340
dc.subjectStatistical Mechanics
dc.subjectMesoscale and Nanoscale Physics
dc.subjectHigh Energy Physics - Theory
dc.titleComment on ``Quantum Statistical Mechanics of an Ideal Gas with Fractional Exclusion Statistics in Arbitrary Dimension"
dc.typetext

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