Constant-density thermodynamic perturbation theory for quantum fluids

B. Kumar and Nutan Chandra

Physica A: Statistical Mechanics and its Applications, 1982, vol. 110, issue 3, 565-579

Abstract: A perturbation series is given which expresses the equilibrium thermodynamic quantities of a quantal fluid in terms of that of another (unperturbed) fluid having the same temperature and number density ρ. The general term of each series can be given; it is the integral of a product involving either the grand-canonical correlation functions of the unperturbed fluid or its fundamental probability distribution WcN(1,…,N) for sets of free particles and the modified Ursell-functions of the quantal fluid; each integral can be conveniently represented in the language of graphs.

Date: 1982
References: View complete reference list from CitEc
Citations:

Downloads: (external link)
http://www.sciencedirect.com/science/article/pii/0378437182900693
Full text for ScienceDirect subscribers only. Journal offers the option of making the article available online on Science direct for a fee of $3,000

Related works:
This item may be available elsewhere in EconPapers: Search for items with the same title.

Export reference: BibTeX RIS (EndNote, ProCite, RefMan) HTML/Text

Persistent link: https://EconPapers.repec.org/RePEc:eee:phsmap:v:110:y:1982:i:3:p:565-579

DOI: 10.1016/0378-4371(82)90069-3

Access Statistics for this article

Physica A: Statistical Mechanics and its Applications is currently edited by K. A. Dawson, J. O. Indekeu, H.E. Stanley and C. Tsallis

More articles in Physica A: Statistical Mechanics and its Applications from Elsevier
Bibliographic data for series maintained by Catherine Liu ().