1997
DOI: 10.1590/s0103-97331997000400025
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On the Nonequilibrium Statistical Operator and Classical Thermofield Dynamics

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Cited by 12 publications
(8 citation statements)
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“…(189), with analytical extension given in Eq. (190). For s = 1 and D = 3, such that ν = s − (D − 2)/2 = 1/2, performing the subtraction of divergent terms, following the procedure of Section 6, and using K ±1/2 (z) = √ πe −z / √ 2z and ∞ n=1 e −ξn /n = − ln(1 − e −ξ ), the self-energy reads…”
mentioning
confidence: 99%
“…(189), with analytical extension given in Eq. (190). For s = 1 and D = 3, such that ν = s − (D − 2)/2 = 1/2, performing the subtraction of divergent terms, following the procedure of Section 6, and using K ±1/2 (z) = √ πe −z / √ 2z and ∞ n=1 e −ξn /n = − ln(1 − e −ξ ), the self-energy reads…”
mentioning
confidence: 99%
“…Este procedimento, que aparece em diversos textos didáticos, fica limitado pela impossibilidade de generalização para sistemas descritos por campos quânticos ou ainda em situações fora do equilíbrio. O procedimento variacional de Tisza é que foi utilizado nas teorias de campos, assim como foi, por exemplo, empregado por Zubarev para descrever processos fora do equilíbrio [35][36][37].…”
Section: O Princípio De Extremo De Tisza E Os Ensembles De Gibbs-einsunclassified
“…Furthermore, the TFD vector space has been taken as a representation space for Lie algebras [15]. Thus, the equations of motion in TFD have been derived from a study of the Galilei and Poincaré symmetries [15,16]; Liouville-von Neumann equations have been introduced for the Klein-Gordan and Dirac field associated with the kinetic theory [17]; and a classical counterpart of TFD has been identified [18,19]. A constitutive element of this representation theory for Lie algebras is the doubling structure in the set of mappings defined in the TFD Hilbert space (actually, this doubling is present in any field formalism dealing with thermal phenomena [1]).…”
Section: Introductionmentioning
confidence: 99%