1970
DOI: 10.1007/bf01646630
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On a class of equilibrium states under the Kubo-Martin-Schwinger condition

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Cited by 43 publications
(30 citation statements)
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“…dp{x) = j (P dpj(p). we get a result, which is a slight generalization of one in [4] and analogous to one in [18], [8]. …”
Section: The Central Decomposition Of Gauge-invariant Quasi-free Statessupporting
confidence: 64%
“…dp{x) = j (P dpj(p). we get a result, which is a slight generalization of one in [4] and analogous to one in [18], [8]. …”
Section: The Central Decomposition Of Gauge-invariant Quasi-free Statessupporting
confidence: 64%
“…Following [25] we replace all V i in this condition by 1 N N −1 k=0 T k x V i and take the limit N → ∞. Then by (6.7), Lemma 5.1(vi), and the ergodic theorem one has β i β k f (V k − V i ) ≥ 0, hence f is of positive type (the remaining conditions, f (0) = 1 and f (V ) = f (−V ), are obviously satisfied).…”
Section: Vacuum Versus Regular Positive Energy Representationsmentioning
confidence: 99%
“…As a starting point for further development, we analyse in details the case of quasi-free states (Section III). Although basic structural results characterizing quasi-free thermal states have been obtained long time ago [28,29,30], we present new (in our opinion simpler) proof of the theorem giving general form of a quasi-free state satisfying the KMS condition (see Theorem 3.1 and 3.7). Section 3.4 contains complete characterizations of stochastically positive quasi-free KMS states and corresponding periodic stochastic processes.…”
Section: Introductionmentioning
confidence: 90%