1977
DOI: 10.1016/0034-4877(77)90078-7
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Integral representations of the classical KMS-states for quasi-free evolutions

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Cited by 7 publications
(5 citation statements)
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“…in some weak sense, see e.g. [3]. These ideas were exploited to construct a various truncations of the full interacting boson Hamiltonian.…”
Section: Motivationmentioning
confidence: 99%
“…in some weak sense, see e.g. [3]. These ideas were exploited to construct a various truncations of the full interacting boson Hamiltonian.…”
Section: Motivationmentioning
confidence: 99%
“…where a(f ) = f (x)a(x)dx for f ∈ C ∞ 0 (R ν ), f is the Fourier transform of f and ρ 0 is the condensate density. It is proved in [20] that (13) implies, amongst other things, the breaking of the gauge symmetry.…”
Section: The Model and Equilibrium Statesmentioning
confidence: 99%
“…In the seventies, G. Gallavotti and E. Verboven, suggested a classical analogue to the quantum KMS condition suitable for classical mechanical systems and they analysed its relationship with the Dobrushin-Lanford-Ruelle (DLR) equation, see [33] and also [1]. The work of Gallavotti and Verboven generated interest in the study of KMS states for infinite classical systems (see for instance [26,54] and the references therein). To the best of our knowledge, only few results are concerned with nonlinear PDEs, namely [9,24,53].…”
Section: Introductionmentioning
confidence: 99%