Abstract
Using the Kubo-Martin-Schwinger boundary condition for equilibrium states of quantum statistical mechanics of fermion gas, we prove that forT≠;0 a one-particle evolution (corresponding essentially to bilinear hamiltonians) generally defines a unique equilibrium state, which is quasi-free. Conversely any quasi-free state is the equilibrium state for a single one-particle evolution if it has no Fock part in its product decomposition. Limiting cases whereT → 0 andT → ∞ are studied. In the case whereT → 0 one shows that the state generally converges to a Fock state linked to the evolution.
Similar content being viewed by others
References
Balslev, E., J. Manuceau, andA. Verbeure: Comm. math. Phys.8, 315 (1968).
Rocca, F., M. Sirugue, andD. Testard: Ann. Inst. H. Poincaré3, 247 (1969).
Haag, R., N. M. Hugenholtz, andM. Winnink: Comm. math. Phys.5, 215 (1967).
Kastler, D., J. C. T. Pool, andE. Thue Poulsen: Comm. Math. Phys.12, 175 (1969).
Powers, R. T.: Thesis, Princeton University 1967.
Manuceau, J., F. Rocca, andD. Testard: Comm. math. Phys.12, 43 (1969).
Hugenholtz, N. M.: Comm. math. Phys.6, 189 (1967).
Kadanoff, L. P., andG. Bayn: Quantum Statistical Mechanics. New York: Benjamin 1962.
Winnink, M.: Thesis, Groningen 1968.
Nelson, E.: Ann. math.70, 572 (1959).
Author information
Authors and Affiliations
Additional information
Attaché de Recherche au C.N.R.S.
This work is a part of a “Thèse de Doctorat d'Etat” presented to the “Faculté des Sciences de Marseille”, April 23, 1969, under the number A.O. 3073.
Rights and permissions
About this article
Cite this article
Rocca, F., Sirugue, M. & Testard, D. On a class of equilibrium states under the Kubo-Martin-Schwinger boundary condition. Commun.Math. Phys. 13, 317–334 (1969). https://doi.org/10.1007/BF01645416
Received:
Revised:
Issue Date:
DOI: https://doi.org/10.1007/BF01645416