{"@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/1361699995243926656.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1016/j.nuclphysb.2014.03.017"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:S0550321314000911?httpAccept=text/xml"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:S0550321314000911?httpAccept=text/plain"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.1401.0466"}}],"dc:title":[{"@value":"The formulation of gauge-Higgs unification with dynamical boundary conditions"}],"description":[{"notation":[{"@value":"The boundary conditions on multiply connected extra dimensions play major rolls in gauge-Higgs unification theory. Different boundary conditions, having been given in ad hoc manner so far, lead to different theories. To solve this arbitrariness problem of boundary conditions, we construct a formulation of gauge-Higgs unification with dynamics of boundary conditions on M^4 times S^1/Z_2. As a result, it is found that only highly restricted sets of boundary conditions, which lead to nontrivial symmetry breaking, practically contribute to the partition function. In particular, we show that for $SU(5)$ gauge group, sets of boundary conditions which lead to SU(5) to SU(3) times SU(2) times U(1) symmetry breaking are naturally included in the restricted sets."}]},{"notation":[{"@value":"19 pages. The discussion in section 3 was changed, Some typos and expressions have been corrected"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1381699995243926656","@type":"Researcher","foaf:name":[{"@value":"Kengo Yamamoto"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"05503213"}],"prism:publicationName":[{"@value":"Nuclear Physics B"}],"dc:publisher":[{"@value":"Elsevier BV"}],"prism:publicationDate":"2014-06","prism:volume":"883","prism:startingPage":"45","prism:endingPage":"58"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["https://www.elsevier.com/tdm/userlicense/1.0/","https://www.elsevier.com/legal/tdmrep-license","http://creativecommons.org/licenses/by/3.0/"],"url":[{"@id":"https://api.elsevier.com/content/article/PII:S0550321314000911?httpAccept=text/xml"},{"@id":"https://api.elsevier.com/content/article/PII:S0550321314000911?httpAccept=text/plain"}],"createdAt":"2014-03-24","modifiedAt":"2025-10-09","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Theory","dc:title":"High Energy Physics - Theory"},{"@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=High%20Energy%20Physics%20-%20Theory%20(hep-th)","dc:title":"High Energy Physics - Theory (hep-th)"},{"@id":"https://cir.nii.ac.jp/all?q=FOS:%20Physical%20sciences","dc:title":"FOS: Physical sciences"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360285709996019328","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>H</mml:mi><mml:mo stretchy=\"false\">→</mml:mo><mml:mi>Z</mml:mi><mml:mi>γ</mml:mi></mml:math>in the gauge-Higgs unification"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285709999053440","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Collider signals of \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>W</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:math>\n and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>Z</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:math>\n bosons in the gauge-Higgs unification"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285711139361664","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Gauge-Higgs EW and grand unification"}]},{"@id":"https://cir.nii.ac.jp/crid/2050307417114079744","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Toward realistic gauge-Higgs grand unification"}]},{"@id":"https://cir.nii.ac.jp/crid/2050588892091749248","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Gauge-Higgs seesaw mechanism in 6-dimensional grand unification"}]},{"@id":"https://cir.nii.ac.jp/crid/2050870367067465728","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Gauge-Higgs grand unification"}]},{"@id":"https://cir.nii.ac.jp/crid/2051151842044118912","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Dark matter in the SO(5) × U(1) gauge-Higgs unification"}]},{"@id":"https://cir.nii.ac.jp/crid/2051433317021905280","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Electroweak symmetry breaking and mass spectra in six-dimensional gauge-Higgs grand unification"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1016/j.nuclphysb.2014.03.017"},{"@type":"OPENAIRE","@value":"doi_dedup___::c6f3c132c88ac9554f6e9a098ea66ca1"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptu146_references_DOI_2EKVdriGEn8w6aYXegSUbtGAOir"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptw116_references_DOI_2EKVdriGEn8w6aYXegSUbtGAOir"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptx124_references_DOI_2EKVdriGEn8w6aYXegSUbtGAOir"},{"@type":"CROSSREF","@value":"10.1103/physrevd.92.115003_references_DOI_2EKVdriGEn8w6aYXegSUbtGAOir"},{"@type":"CROSSREF","@value":"10.1103/physrevd.95.035032_references_DOI_2EKVdriGEn8w6aYXegSUbtGAOir"},{"@type":"CROSSREF","@value":"10.1142/s0217751x16300313_references_DOI_2EKVdriGEn8w6aYXegSUbtGAOir"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptv153_references_DOI_2EKVdriGEn8w6aYXegSUbtGAOir"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptx175_references_DOI_2EKVdriGEn8w6aYXegSUbtGAOir"}]}