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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 wikiPageLength "5990".
- KMS_state wikiPageOutDegree "34".
- KMS_state wikiPageRevisionID "665477333".
- KMS_state wikiPageWikiLink Analytic_function.
- KMS_state wikiPageWikiLink Category:Quantum_field_theory.
- KMS_state wikiPageWikiLink Category:Statistical_mechanics.
- KMS_state wikiPageWikiLink Charge_(physics).
- KMS_state wikiPageWikiLink Complex-valued_function.
- KMS_state wikiPageWikiLink Complex_function.
- KMS_state wikiPageWikiLink Conservation_law.
- KMS_state wikiPageWikiLink Conservation_law_(physics).
- KMS_state wikiPageWikiLink Density_matrix.
- KMS_state wikiPageWikiLink Distribution_(mathematics).
- KMS_state wikiPageWikiLink Expected_value.
- KMS_state wikiPageWikiLink Greens_function.
- KMS_state wikiPageWikiLink Hagedorn_temperature.
- KMS_state wikiPageWikiLink Hamiltonian_(quantum_mechanics).
- KMS_state wikiPageWikiLink Heisenberg_picture.
- KMS_state wikiPageWikiLink Hilbert_space.
- KMS_state wikiPageWikiLink Internal_symmetry.
- KMS_state wikiPageWikiLink Journal_of_the_Physical_Society_of_Japan.
- KMS_state wikiPageWikiLink Julian_Schwinger.
- KMS_state wikiPageWikiLink Local_symmetry.
- KMS_state wikiPageWikiLink Operator_(physics).
- KMS_state wikiPageWikiLink Particle_number_operator.
- KMS_state wikiPageWikiLink Partition_function_(quantum_field_theory).
- KMS_state wikiPageWikiLink Phase_transition.
- KMS_state wikiPageWikiLink Physical_Review.
- KMS_state wikiPageWikiLink Quantum_field_theory.
- KMS_state wikiPageWikiLink Quantum_mechanics.
- KMS_state wikiPageWikiLink Ryogo_Kubo.
- KMS_state wikiPageWikiLink Spectrum_(functional_analysis).
- KMS_state wikiPageWikiLink Spectrum_of_an_operator.
- KMS_state wikiPageWikiLink Spontaneous_symmetry_breaking.
- KMS_state wikiPageWikiLink Statistical_mechanics.
- KMS_state wikiPageWikiLink Thermodynamic.
- KMS_state wikiPageWikiLink Thermodynamics.
- KMS_state wikiPageWikiLink Tomita–Takesaki_theory.
- KMS_state wikiPageWikiLink Trace_class.
- KMS_state wikiPageWikiLink Unitary_transformation.
- KMS_state wikiPageWikiLinkText "KMS (Kubo-Martin-Schwinger) condition".
- KMS_state wikiPageWikiLinkText "KMS state".
- KMS_state wikiPageWikiLinkText "KMS theory".
- 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 wikiPageUsesTemplate Template:Citation.
- KMS_state wikiPageUsesTemplate Template:Harvs.
- KMS_state wikiPageUsesTemplate Template:Harvtxt.
- KMS_state year "1967".
- KMS_state subject Category:Quantum_field_theory.
- KMS_state subject Category:Statistical_mechanics.
- KMS_state type Mechanic.
- KMS_state type Physic.
- 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 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=665477333.
- KMS_state isPrimaryTopicOf KMS_state.