
arXiv: hep-th/9904049
We show that the Reeh–Schlieder property w.r.t. KMS states is a direct consequence of locality, additivity, and the relativistic KMS condition. The latter characterizes the thermal equilibrium states of a relativistic quantum field theory. The statement remains valid even if the given equilibrium state breaks spatial translation invariance.
High Energy Physics - Theory, KMS states, locality, additivity, Applications of operator algebras to the sciences, High Energy Physics - Theory (hep-th), Applications of selfadjoint operator algebras to physics, Applications of operator theory in the physical sciences, FOS: Physical sciences, Quantum equilibrium statistical mechanics (general), Axiomatic quantum field theory; operator algebras
High Energy Physics - Theory, KMS states, locality, additivity, Applications of operator algebras to the sciences, High Energy Physics - Theory (hep-th), Applications of selfadjoint operator algebras to physics, Applications of operator theory in the physical sciences, FOS: Physical sciences, Quantum equilibrium statistical mechanics (general), Axiomatic quantum field theory; operator algebras
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