1977
DOI: 10.1007/bf01315509
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Operator orderings and functional formulations of quantum and stochastic dynamics

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Cited by 55 publications
(21 citation statements)
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“…This approach has been first developed for cases with an additive noise [45,46,47,48,49,50]. It was later generalised to cases with a multiplicative noise [6] and extended to various discretization schemes and to higher dimensions [7,8]. Below, we recall the construction of such a path-integral representation on the case of the multiplicative-noise equation (2.1) by following a procedureà la MartinSiggia-Rose-Janssen-deDominicis (MSRJD).…”
Section: The Path-integral Formulationmentioning
confidence: 99%
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“…This approach has been first developed for cases with an additive noise [45,46,47,48,49,50]. It was later generalised to cases with a multiplicative noise [6] and extended to various discretization schemes and to higher dimensions [7,8]. Below, we recall the construction of such a path-integral representation on the case of the multiplicative-noise equation (2.1) by following a procedureà la MartinSiggia-Rose-Janssen-deDominicis (MSRJD).…”
Section: The Path-integral Formulationmentioning
confidence: 99%
“…2.3 we recall the path-integral generating-functional formalism for stochastic Langevin processes with multiplicative white noise [6,7,8,9,10,11]. We explain the apparent differences with the path integrals used in Ref.…”
Section: Contents 1 Introductionmentioning
confidence: 99%
“…где V e (t) берется в картине евклидова взаимодействия (6). Для оператора эволюции U (t i , t f ) из-за наличия упорядоченных по времени аргументов (t f > t i ) представле-ние, полученное с использованием антихронологически упорядоченной экспоненты, имеет вид…”
Section: зависящие от времени функции грина при конечной температуреunclassified
“…Кроме обычных квантово-механических задач, важные стохастические задачи можно сформулировать в терминах полевых операторов, аналогичных операторам квантовой теории поля [5], [6], которые порождают функции Грина, определенные по аналогии с (1). Основное отличие от функций Грина квантовой теории поля со-стоит в виде оператора плотности, который в случае стохастических задач построен существенно отличающимся от (2) или (3) путем.…”
Section: Introductionunclassified
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