Schwinger-Dyson BRST symmetry and the equivalence of Hamiltonian and Lagrangian quantisation

Implementing the requirement that a field theory be invariant under Schwinger-Dyson BRST symmetry in the Hamiltonian formalism, we show the equivalence between Hamiltonian and Lagrangian BRST-formalism at the path integral level. The Lagrangian quantum master equation is derived as a direct conseque...

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Detalles Bibliográficos
Autor principal: De Jonghe, Frank
Lenguaje:eng
Publicado: 1993
Materias:
General Theoretical Physics
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(93)91035-L
http://cds.cern.ch/record/246807
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author De Jonghe, Frank
author_facet De Jonghe, Frank
author_sort De Jonghe, Frank
collection CERN
description Implementing the requirement that a field theory be invariant under Schwinger-Dyson BRST symmetry in the Hamiltonian formalism, we show the equivalence between Hamiltonian and Lagrangian BRST-formalism at the path integral level. The Lagrangian quantum master equation is derived as a direct consequence of the Fradkin-Vilkovisky theorem in Hamiltonian BRST quantisation.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1993
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spelling cern-2468072023-03-14T19:27:30Zdoi:10.1016/0370-2693(93)91035-Lhttp://cds.cern.ch/record/246807engDe Jonghe, FrankSchwinger-Dyson BRST symmetry and the equivalence of Hamiltonian and Lagrangian quantisationGeneral Theoretical PhysicsImplementing the requirement that a field theory be invariant under Schwinger-Dyson BRST symmetry in the Hamiltonian formalism, we show the equivalence between Hamiltonian and Lagrangian BRST-formalism at the path integral level. The Lagrangian quantum master equation is derived as a direct consequence of the Fradkin-Vilkovisky theorem in Hamiltonian BRST quantisation.Implementing the requirement that a field theory be invariant under Schwinger-Dyson BRST symmetry in the Hamiltonian formalism, we show the equivalence between Hamiltonian and Lagrangian BRST-formalism at the path integral level. The Lagrangian quantum master equation is derived as a direct consequence of the Fradkin-Vilkovisky theorem in Hamiltonian BRST quantisation.Implementing the requirement that a field theory be invariant under Schwinger-Dyson BRST symmetry in the Hamiltonian formalism, we show the equivalence between Hamiltonian and Lagrangian BRST formalism at the path integral level. The Lagrangian quantum master equation is derived as a direct consequence of the Fradkin-Vilkovisky theorem in Hamiltonian BRST quantisation.hep-th/9303027KUL-TF-93-08CERN-TH-6823-93CERN-TH-6823-93KUL-TF-93-08oai:cds.cern.ch:2468071993
spellingShingle General Theoretical Physics
De Jonghe, Frank
Schwinger-Dyson BRST symmetry and the equivalence of Hamiltonian and Lagrangian quantisation
title Schwinger-Dyson BRST symmetry and the equivalence of Hamiltonian and Lagrangian quantisation
title_full Schwinger-Dyson BRST symmetry and the equivalence of Hamiltonian and Lagrangian quantisation
title_fullStr Schwinger-Dyson BRST symmetry and the equivalence of Hamiltonian and Lagrangian quantisation
title_full_unstemmed Schwinger-Dyson BRST symmetry and the equivalence of Hamiltonian and Lagrangian quantisation
title_short Schwinger-Dyson BRST symmetry and the equivalence of Hamiltonian and Lagrangian quantisation
title_sort schwinger-dyson brst symmetry and the equivalence of hamiltonian and lagrangian quantisation
topic General Theoretical Physics
url https://dx.doi.org/10.1016/0370-2693(93)91035-L
http://cds.cern.ch/record/246807
work_keys_str_mv AT dejonghefrank schwingerdysonbrstsymmetryandtheequivalenceofhamiltonianandlagrangianquantisation

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