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- KMS_state abstract "In the statistical mechanics of quantum mechanical systems and quantum field theory, the properties of a system in thermal equilibrium can be described by a mathematical object called a Kubo-Martin-Schwinger state or, more commonly, a KMS state: a state satisfying the KMS condition. Kubo (1957) introduced the condition, Martin & Schwinger (1959) used it to define thermodynamic Greens functions, and Rudolf Haag, M. Winnink, and N. M. Hugenholtz (1967) used the condition to define equilibrium states and called it the KMS condition.".
- KMS_state wikiPageID "2834214".
- KMS_state wikiPageRevisionID "605281703".
- KMS_state author1Link "Rudolf Haag".
- KMS_state first "M.".
- KMS_state first "N. M.".
- KMS_state first "Rudolf".
- KMS_state hasPhotoCollection KMS_state.
- KMS_state last "Haag".
- KMS_state last "Hugenholtz".
- KMS_state last "Winnink".
- KMS_state year "1967".
- KMS_state subject Category:Quantum_field_theory.
- KMS_state subject Category:Statistical_mechanics.
- KMS_state comment "In the statistical mechanics of quantum mechanical systems and quantum field theory, the properties of a system in thermal equilibrium can be described by a mathematical object called a Kubo-Martin-Schwinger state or, more commonly, a KMS state: a state satisfying the KMS condition. Kubo (1957) introduced the condition, Martin & Schwinger (1959) used it to define thermodynamic Greens functions, and Rudolf Haag, M. Winnink, and N. M.".
- KMS_state label "KMS state".
- KMS_state label "KMS状態".
- KMS_state label "État KMS".
- KMS_state sameAs État_KMS.
- KMS_state sameAs KMS状態.
- KMS_state sameAs m.085pxm.
- KMS_state sameAs Q3591812.
- KMS_state sameAs Q3591812.
- KMS_state wasDerivedFrom KMS_state?oldid=605281703.
- KMS_state isPrimaryTopicOf KMS_state.