{"@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/1363670318625506432.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1016/0370-2693(96)00446-7"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:0370269396004467?httpAccept=text/xml"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:0370269396004467?httpAccept=text/plain"}}],"dc:title":[{"@value":"The next-to-minimal Coleman-Weinberg model"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1383670318625506432","@type":"Researcher","foaf:name":[{"@value":"Ralf Hempfling"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"03702693"}],"prism:publicationName":[{"@value":"Physics Letters B"}],"dc:publisher":[{"@value":"Elsevier BV"}],"prism:publicationDate":"1996-06","prism:volume":"379","prism:number":"1-4","prism:startingPage":"153","prism:endingPage":"158"},"reviewed":"false","dc:rights":["https://www.elsevier.com/tdm/userlicense/1.0/"],"url":[{"@id":"https://api.elsevier.com/content/article/PII:0370269396004467?httpAccept=text/xml"},{"@id":"https://api.elsevier.com/content/article/PII:0370269396004467?httpAccept=text/plain"}],"createdAt":"2002-07-26","modifiedAt":"2019-04-17","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360002217828920448","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Probing a classically conformal \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>B</mml:mi><mml:mo>−</mml:mo><mml:mi>L</mml:mi></mml:math>\n model with gravitational waves"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004231125671168","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"A scale-invariant Higgs sector and structure of the vacuum"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004231136914688","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Electroweak and conformal symmetry  breaking by a strongly coupled hidden sector"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235015138688","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Radiative symmetry breaking from flat potential in various<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>U</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>1</mml:mn><mml:msup><mml:mrow><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>models"}]},{"@id":"https://cir.nii.ac.jp/crid/1360009142621638528","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Heavy dark matter, neutrino masses, and Higgs naturalness from a strongly interacting hidden sector"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706097616384","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Gauge coupling unification in a classically scale invariant model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285707418981504","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"A new dynamics of electroweak symmetry breaking with classically scale invariance"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285709991646848","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Radiative symmetry breaking at the Fermi scale and flat potential at the Planck scale"}]},{"@id":"https://cir.nii.ac.jp/crid/1360294643773200512","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Unified emergence of energy scales and cosmic inflation"}]},{"@id":"https://cir.nii.ac.jp/crid/1360294647607570176","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Planck and Electroweak Scales Emerging from Conformal Gravity"}]},{"@id":"https://cir.nii.ac.jp/crid/1360565167406892288","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Scale genesis and gravitational wave in a classically scale invariant extension of the standard model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567181083935744","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Gamma-ray line from Nambu-Goldstone dark matter in a scale invariant extension of the Standard Model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567182360025216","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Physics beyond the standard model may be described by a massless QFT"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567182395631232","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Bosonic seesaw mechanism in a classically conformal extension of the Standard Model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184971271168","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Nambu-Goldstone dark matter in a scale invariant bright hidden sector"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184975396096","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Invisible axionlike dark matter from the electroweak bosonic seesaw mechanism"}]},{"@id":"https://cir.nii.ac.jp/crid/2050588892091798400","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Left-right symmetry, orbifold S1/Z2, and radiative breaking of U(1)R × U(1)B-L"}]},{"@id":"https://cir.nii.ac.jp/crid/2051996266974303360","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Scale and electroweak first-order phase transitions"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1016/0370-2693(96)00446-7"},{"@type":"CROSSREF","@value":"10.1103/physrevd.95.015020_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1007/jhep05(2015)030_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2013)076_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1093/ptep/pty095_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1103/physrevd.89.056010_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1016/j.physletb.2016.02.052_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1103/physrevd.102.035026_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1007/jhep02(2016)058_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1103/physrevd.89.016019_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1007/jhep08(2021)016_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1088/1475-7516/2016/12/001_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1007/jhep09(2014)016_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1103/physrevd.91.115007_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1103/physrevd.94.095011_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptv114_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1140/epjc/s10052-018-6289-8_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1016/j.nuclphysb.2018.01.013_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"},{"@type":"CROSSREF","@value":"10.1016/j.physletb.2016.01.050_references_DOI_88RLydlXPzwViqbo7Iw2fisoGD0"}]}