Abstract:
The partition function for the electron gas in the field of arbitrarily positioned protons
is calculated. The free energy of the system is represented in the form of quantum
virial expansions for the electron subsystem and the energy of the many-particle
effective interactions of the protons.
Citation:
M. V. Vavrukh, “Partition function of the hydrogen system in the metallic state”, TMF, 36:3 (1978), 400–413; Theoret. and Math. Phys., 36:3 (1978), 816–824
\Bibitem{Vav78}
\by M.~V.~Vavrukh
\paper Partition function of the hydrogen system in the metallic state
\jour TMF
\yr 1978
\vol 36
\issue 3
\pages 400--413
\mathnet{http://mi.mathnet.ru/tmf3089}
\transl
\jour Theoret. and Math. Phys.
\yr 1978
\vol 36
\issue 3
\pages 816--824
\crossref{https://doi.org/10.1007/BF01035757}
Linking options:
https://www.mathnet.ru/eng/tmf3089
https://www.mathnet.ru/eng/tmf/v36/i3/p400
This publication is cited in the following 3 articles:
I. V. Pylyuk, “Critical behavior of the three-dimensional Ising sistem: Dependence of themodynamic characteristics on microscopic parameters”, Theoret. and Math. Phys., 117:3 (1998), 1459–1482
M. V. Vavrukh, “n-Particle correlation functions of an interacting electron gas”, Theoret. and Math. Phys., 50:3 (1982), 288–296
M. V. Vavrukh, T. E. Krokhmal'skii, “Effective many-particle interactions of ions in metals”, Theoret. and Math. Phys., 51:1 (1982), 400–408
Citation in format AMSBIB
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