{"@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/1360011143499558016.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1016/0550-3213(94)90543-6"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:0550321394905436?httpAccept=text/xml"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:0550321394905436?httpAccept=text/plain"}}],"dc:title":[{"@value":"Effective average action for gauge theories and exact evolution equations"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380011143499558017","@type":"Researcher","foaf:name":[{"@value":"M. Reuter"}]},{"@id":"https://cir.nii.ac.jp/crid/1380011143499558016","@type":"Researcher","foaf:name":[{"@value":"C. Wetterich"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"05503213"}],"prism:publicationName":[{"@value":"Nuclear Physics B"}],"dc:publisher":[{"@value":"Elsevier BV"}],"prism:publicationDate":"1994-04","prism:volume":"417","prism:number":"1-2","prism:startingPage":"181","prism:endingPage":"214"},"reviewed":"false","dc:rights":["https://www.elsevier.com/tdm/userlicense/1.0/"],"url":[{"@id":"https://api.elsevier.com/content/article/PII:0550321394905436?httpAccept=text/xml"},{"@id":"https://api.elsevier.com/content/article/PII:0550321394905436?httpAccept=text/plain"}],"createdAt":"2002-11-12","modifiedAt":"2020-03-11","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360013168734706560","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Higgs scalar potential coupled to gravity in the exponential parametrization in arbitrary gauge"}]},{"@id":"https://cir.nii.ac.jp/crid/1360025431135547392","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Functional renormalization group study of a four-fermion model with \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>C</mml:mi><mml:mi>P</mml:mi></mml:math>\n violation"}]},{"@id":"https://cir.nii.ac.jp/crid/1361694365613033216","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Functional renormalization group approach to color superconducting phase transition"}]},{"@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/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":"10.1016/0550-3213(94)90543-6"},{"@type":"CROSSREF","@value":"10.1143/ptp.120.197_references_DOI_S47i3MwDg3BNvGiK57oQ1m2vHru"},{"@type":"CROSSREF","@value":"10.1103/physrevd.105.026013_references_DOI_S47i3MwDg3BNvGiK57oQ1m2vHru"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptac003_references_DOI_S47i3MwDg3BNvGiK57oQ1m2vHru"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptac047_references_DOI_S47i3MwDg3BNvGiK57oQ1m2vHru"},{"@type":"CROSSREF","@value":"10.1103/physrevd.111.074015_references_DOI_S47i3MwDg3BNvGiK57oQ1m2vHru"},{"@type":"CROSSREF","@value":"10.1143/ptp.106.149_references_DOI_S47i3MwDg3BNvGiK57oQ1m2vHru"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2019)069_references_DOI_S47i3MwDg3BNvGiK57oQ1m2vHru"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptz099_references_DOI_S47i3MwDg3BNvGiK57oQ1m2vHru"}]}