Selfconsistent random phase approximation for hot finite Fermi-systems
Teoretičeskaâ i matematičeskaâ fizika, Tome 111 (1997) no. 2, pp. 279-288

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By using a formalism of thermofield dynamics a new approach with the account of the influence of temperature and collective motion parameters on a mean field in hot finite Fermi-systems like atomic nuclei and metallic clusters is elaborated. Within the approach Pauli principle effects are considered in more correct way than in the standard termal random phase approximation.
@article{TMF_1997_111_2_a8,
     author = {A. I. Vdovin and D. S. Kosov and W. Nawrocka},
     title = {Selfconsistent random phase approximation for hot finite {Fermi-systems}},
     journal = {Teoreti\v{c}eska\^a i matemati\v{c}eska\^a fizika},
     pages = {279--288},
     publisher = {mathdoc},
     volume = {111},
     number = {2},
     year = {1997},
     language = {ru},
     url = {http://geodesic.mathdoc.fr/item/TMF_1997_111_2_a8/}
}
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A. I. Vdovin; D. S. Kosov; W. Nawrocka. Selfconsistent random phase approximation for hot finite Fermi-systems. Teoretičeskaâ i matematičeskaâ fizika, Tome 111 (1997) no. 2, pp. 279-288. http://geodesic.mathdoc.fr/item/TMF_1997_111_2_a8/