KMS state (original) (raw)
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. introduced the condition, used it to define thermodynamic Green's functions, and Rudolf Haag, M. Winnink, and N. M. Hugenholtz used the condition to define equilibrium states and called it the KMS condition.
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| dbo: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. introduced the condition, used it to define thermodynamic Green's functions, and Rudolf Haag, M. Winnink, and N. M. Hugenholtz used the condition to define equilibrium states and called it the KMS condition. (en) Dans la mécanique quantique et la théorie quantique des champs, la propriété d'un système en équilibre thermique peut être décrite par un objet mathématique appelé état Kubo-Martin-Schwinger ou plus simplement état KMS : un état satisfaisant la condition KMS. Kubo établit les premières bases en 1957, Martin et Schwinger utilisèrent cet état pour définir des fonctions de Green thermodynamiques en 1959. (fr) 함수해석학과 양자역학에서 구보-마틴-슈윙거 상태([久保]-Martin-Schwinger狀態, 영어: Kubo–Martin–Schwinger state, 약자 KMS 상태)는 특정하게 열역학적 평형을 이룬 순수 또는 혼합 상태이다. (ko) 量子力学や場の量子論の系の統計力学では、熱平衡状態にある系の性質を数学的な対象で記述することができて、久保-マーティン-シュウィンガー状態(KMS state)、一般には KMS状態 と呼ばれる。この状態は、 で導入された KMS条件(KMS condition）を満たし、ではこれを使い 熱力学的 グリーン函数 を定義し、, M. Winnink, and N. M. Hugenholtz は熱平衡状態を定義することに使った。 (ja) |
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| dbp:author1Link | Rudolf Haag (en) |
| dbp:authorlink | Nicolaas Marinus Hugenholtz (en) |
| dbp:first | M. (en) Rudolf (en) N. M. (en) |
| dbp:last | Haag (en) Hugenholtz (en) Winnink (en) |
| dbp:wikiPageUsesTemplate | dbt:Citation dbt:Expert_needed dbt:Harvtxt dbt:Quantum-stub dbt:Short_description dbt:Harvs |
| dbp:year | 1967 (xsd:integer) |
| dct:subject | dbc:Quantum_field_theory dbc:Statistical_mechanics |
| rdfs: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. introduced the condition, used it to define thermodynamic Green's functions, and Rudolf Haag, M. Winnink, and N. M. Hugenholtz used the condition to define equilibrium states and called it the KMS condition. (en) Dans la mécanique quantique et la théorie quantique des champs, la propriété d'un système en équilibre thermique peut être décrite par un objet mathématique appelé état Kubo-Martin-Schwinger ou plus simplement état KMS : un état satisfaisant la condition KMS. Kubo établit les premières bases en 1957, Martin et Schwinger utilisèrent cet état pour définir des fonctions de Green thermodynamiques en 1959. (fr) 함수해석학과 양자역학에서 구보-마틴-슈윙거 상태([久保]-Martin-Schwinger狀態, 영어: Kubo–Martin–Schwinger state, 약자 KMS 상태)는 특정하게 열역학적 평형을 이룬 순수 또는 혼합 상태이다. (ko) 量子力学や場の量子論の系の統計力学では、熱平衡状態にある系の性質を数学的な対象で記述することができて、久保-マーティン-シュウィンガー状態(KMS state)、一般には KMS状態 と呼ばれる。この状態は、 で導入された KMS条件(KMS condition）を満たし、ではこれを使い 熱力学的 グリーン函数 を定義し、, M. Winnink, and N. M. Hugenholtz は熱平衡状態を定義することに使った。 (ja) |
| rdfs:label | État KMS (fr) KMS state (en) KMS状態 (ja) 구보-마틴-슈윙거 상태 (ko) |
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