{"@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/1362262943839330176.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1142/s0217751x01004554"}},{"identifier":{"@type":"URI","@value":"https://www.worldscientific.com/doi/pdf/10.1142/S0217751X01004554"}}],"dc:title":[{"@value":"AN EXACT RG FORMULATION OF QUANTUM GAUGE THEORY"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:p> A gauge invariant Wilsonian effective action is constructed for pure SU(N) Yang-Mills theory by formulating the corresponding flow equation. Manifestly gauge invariant calculations can be performed i.e. without gauge fixing or ghosts. Regularisation is implemented in a novel way which realises a spontaneously broken SU(N|N) supergauge theory. As an example we sketch the computation of the one-loop β function, performed for the first time without any gauge fixing. </jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1382262943839330176","@type":"Researcher","foaf:name":[{"@value":"T. R. MORRIS"}],"jpcoar:affiliationName":[{"@value":"Department of Physics, University of Southampton, Highfield, Southampton SO17 1BJ, UK"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"0217751X"},{"@type":"EISSN","@value":"1793656X"}],"prism:publicationName":[{"@value":"International Journal of Modern Physics A"}],"dc:publisher":[{"@value":"World Scientific Pub Co Pte Lt"}],"prism:publicationDate":"2001-04-30","prism:volume":"16","prism:number":"11","prism:startingPage":"1899","prism:endingPage":"1911"},"reviewed":"false","url":[{"@id":"https://www.worldscientific.com/doi/pdf/10.1142/S0217751X01004554"}],"createdAt":"2002-07-27","modifiedAt":"2019-08-06","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=Astronomy%20and%20Astrophysics","dc:title":"Astronomy and Astrophysics"},{"@id":"https://cir.nii.ac.jp/all?q=Nuclear%20and%20High%20Energy%20Physics","dc:title":"Nuclear and High Energy Physics"},{"@id":"https://cir.nii.ac.jp/all?q=Atomic%20and%20Molecular%20Physics,%20and%20Optics","dc:title":"Atomic and Molecular Physics, and Optics"}],"relatedProduct":[{"@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/2050025942148304000","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"BRST in the exact renormalization group"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1142/s0217751x01004554"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2019)069_references_DOI_GBGt48Y9nYSKuI09EuyyNj1v3pd"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptz099_references_DOI_GBGt48Y9nYSKuI09EuyyNj1v3pd"}]}