<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-04-14T06:20:19Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2445/24561" metadataPrefix="qdc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2445/24561</identifier><datestamp>2025-12-05T16:56:18Z</datestamp><setSpec>com_2072_1057</setSpec><setSpec>col_2072_478823</setSpec><setSpec>col_2072_478917</setSpec></header><metadata><qdc:qualifieddc xmlns:qdc="http://dspace.org/qualifieddc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://purl.org/dc/elements/1.1/ http://dublincore.org/schemas/xmls/qdc/2006/01/06/dc.xsd http://purl.org/dc/terms/ http://dublincore.org/schemas/xmls/qdc/2006/01/06/dcterms.xsd http://dspace.org/qualifieddc/ http://www.ukoln.ac.uk/metadata/dcmi/xmlschema/qualifieddc.xsd">
   <dc:title>Perturbation theory and locality in the Field-Antifield formalism</dc:title>
   <dc:creator>Gomis Torné, Joaquim</dc:creator>
   <dc:creator>París, Jordi</dc:creator>
   <dc:subject>Física nuclear</dc:subject>
   <dc:subject>Física matemàtica</dc:subject>
   <dc:subject>Pertorbació (Matemàtica)</dc:subject>
   <dc:subject>Camps de galga (Física)</dc:subject>
   <dc:subject>Nuclear physics</dc:subject>
   <dc:subject>Mathematical physics</dc:subject>
   <dc:subject>Perturbation (Mathematics)</dc:subject>
   <dc:subject>Gauge fields (Physics)</dc:subject>
   <dcterms:abstract>The BatalinVilkovisky formalism is studied in the framework of perturbation theory by analyzing the antibracket BecchiRouetStoraTyutin (BRST) cohomology of the proper solution S0. It is concluded that the recursive equations for the complete proper solution S can be solved at any order of perturbation theory. If certain conditions on the classical action and on the gauge generators are imposed the solution can be taken local.</dcterms:abstract>
   <dcterms:issued>2012-04-26T10:18:07Z</dcterms:issued>
   <dcterms:issued>2012-04-26T10:18:07Z</dcterms:issued>
   <dcterms:issued>1993</dcterms:issued>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
   <dc:relation>Reproducció del document proporcionada per AIP i http://dx.doi.org/10.1063/1.530407</dc:relation>
   <dc:relation>Journal of Mathematical Physics, 1993, vol. 34, p. 2132</dc:relation>
   <dc:relation>http://dx.doi.org/10.1063/1.530407</dc:relation>
   <dc:rights>(c) American Institute of Physics, 1993</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:publisher>American Institute of Physics</dc:publisher>
   <dc:source>Articles publicats en revistes (Física Quàntica i Astrofísica)</dc:source>
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