{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1364233268505582976.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1016/0370-2693(94)90365-4"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:0370269394903654?httpAccept=text/xml"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:0370269394903654?httpAccept=text/plain"}}],"dc:title":[{"@value":"Flow equations and BRS invariance for Yang-Mills theories"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1384233268505582976","@type":"Researcher","foaf:name":[{"@value":"Ulrich Ellwanger"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"03702693"}],"prism:publicationName":[{"@value":"Physics Letters B"}],"dc:publisher":[{"@value":"Elsevier BV"}],"prism:publicationDate":"1994-09","prism:volume":"335","prism:number":"3-4","prism:startingPage":"364","prism:endingPage":"370"},"reviewed":"false","dc:rights":["https://www.elsevier.com/tdm/userlicense/1.0/"],"url":[{"@id":"https://api.elsevier.com/content/article/PII:0370269394903654?httpAccept=text/xml"},{"@id":"https://api.elsevier.com/content/article/PII:0370269394903654?httpAccept=text/plain"}],"createdAt":"2002-11-12","modifiedAt":"2019-04-03","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360004235011337472","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Fixed point merger in the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>S</mml:mi><mml:mi>U</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>N</mml:mi><mml:mo stretchy=\"false\">)</mml:mo></mml:math>gauge beta functions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285709430329728","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Gauge invariant composite operators of QED in the exact renormalization group formalism"}]},{"@id":"https://cir.nii.ac.jp/crid/1390282679136261376","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"BRS Symmetry, the Quantum Master Equation and the Wilsonian Renormalization Group."}]},{"@id":"https://cir.nii.ac.jp/crid/1520010379901828480","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Construction of a Wilson action for the Wess-Zumino model"},{"@language":"ja-Kana","@value":"Construction of a Wilson action for the Wess Zumino model"}]},{"@id":"https://cir.nii.ac.jp/crid/2050025942148304000","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"BRST in the exact renormalization group"}]},{"@id":"https://cir.nii.ac.jp/crid/2051151842060140160","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"QED in the exact renormalization group"}]},{"@id":"https://cir.nii.ac.jp/crid/2051151842060147328","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Manifestly gauge invariant exact renormalization group for quantum electrodynamics"}]},{"@id":"https://cir.nii.ac.jp/crid/2051714792015378688","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"One-particle irreducible Wilson action in the gradient flow exact renormalization group formalism"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1016/0370-2693(94)90365-4"},{"@type":"CROSSREF","@value":"10.1143/ptp.120.197_references_DOI_CDHm5QVB91SPEvk886MN8Fu3Rn4"},{"@type":"CROSSREF","@value":"10.1103/physrevd.84.125006_references_DOI_CDHm5QVB91SPEvk886MN8Fu3Rn4"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptab142_references_DOI_CDHm5QVB91SPEvk886MN8Fu3Rn4"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptac003_references_DOI_CDHm5QVB91SPEvk886MN8Fu3Rn4"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptac047_references_DOI_CDHm5QVB91SPEvk886MN8Fu3Rn4"},{"@type":"CROSSREF","@value":"10.1088/1751-8113/47/1/015401_references_DOI_CDHm5QVB91SPEvk886MN8Fu3Rn4"},{"@type":"CROSSREF","@value":"10.1143/ptp.106.149_references_DOI_CDHm5QVB91SPEvk886MN8Fu3Rn4"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptz099_references_DOI_CDHm5QVB91SPEvk886MN8Fu3Rn4"}]}