{"@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/1362825895996735616.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1016/0370-2693(79)90425-8"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:0370269379904258?httpAccept=text/xml"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:0370269379904258?httpAccept=text/plain"}}],"dc:title":[{"@value":"Spontaneous breaking of supersymmetry through dimensional reduction"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380004053896783381","@type":"Researcher","foaf:name":[{"@value":"J. Scherk"}]},{"@id":"https://cir.nii.ac.jp/crid/1382825895996735617","@type":"Researcher","foaf:name":[{"@value":"John H. Schwarz"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"03702693"}],"prism:publicationName":[{"@value":"Physics Letters B"}],"dc:publisher":[{"@value":"Elsevier BV"}],"prism:publicationDate":"1979-03","prism:volume":"82","prism:number":"1","prism:startingPage":"60","prism:endingPage":"64"},"reviewed":"false","dc:rights":["https://www.elsevier.com/tdm/userlicense/1.0/"],"url":[{"@id":"https://api.elsevier.com/content/article/PII:0370269379904258?httpAccept=text/xml"},{"@id":"https://api.elsevier.com/content/article/PII:0370269379904258?httpAccept=text/plain"}],"createdAt":"2002-11-12","modifiedAt":"2019-04-03","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050001202619345152","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Non-geometric backgrounds based on topological interfaces"}]},{"@id":"https://cir.nii.ac.jp/crid/1050001202648303616","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Non-supersymmetric asymmetric orbifolds with vanishing cosmological constant"}]},{"@id":"https://cir.nii.ac.jp/crid/1050001338921941120","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Orbifold family unification on six dimensions"},{"@value":"Orbifold family unification on 6 dimensions"}]},{"@id":"https://cir.nii.ac.jp/crid/1050012570393907200","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Gauge-Higgs unification in Lifshitz-type gauge theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1050282813898697728","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Orbifold family unification in SO(2N) gauge theory"},{"@value":"Orbifold family unification in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>S</mml:mi><mml:mi>O</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>2</mml:mn><mml:mi>N</mml:mi><mml:mo stretchy=\"false\">)</mml:mo></mml:math>gauge theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1050294045370732416","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Operator analysis of physical states on magnetized T2/Z(N) orbifolds"},{"@value":"Operator analysis of physical states on magnetized <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:msup><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo stretchy=\"false\">/</mml:mo><mml:msub><mml:mrow><mml:mi>Z</mml:mi></mml:mrow><mml:mrow><mml:mi>N</mml:mi></mml:mrow></mml:msub></mml:math> orbifolds"}]},{"@id":"https://cir.nii.ac.jp/crid/1050294045371382272","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Z N twisted orbifold models with magnetic flux"}]},{"@id":"https://cir.nii.ac.jp/crid/1050564285788993664","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Classification of three-generation models on magnetized orbifolds"}]},{"@id":"https://cir.nii.ac.jp/crid/1050564288879620736","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"CLASSIFICATION OF STANDARD MODEL PARTICLES IN E-6 ORBIFOLD GRAND UNIFIED THEORIES"},{"@value":"CLASSIFICATION OF STANDARD MODEL PARTICLES IN E<sub>6</sub>ORBIFOLD GRAND UNIFIED THEORIES"}]},{"@id":"https://cir.nii.ac.jp/crid/1050585426675831168","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Stability, enhanced gauge symmetry and suppressed cosmological constant in 9D heterotic interpolating models"},{"@language":"ja-Kana","@value":"9ジゲン ヘテロガタ ナイソウ ゲン モケイ ニオケル アンテイナ シンクウ ゲージ タイショウセイ ノ カクダイ ウチュウコウ ノ ヨクセイ"},{"@language":"ja","@value":"9次元ヘテロ型内挿弦模型における安定な真空、ゲージ対称性の拡大、宇宙項の抑制"}]},{"@id":"https://cir.nii.ac.jp/crid/1050845763852101248","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"SOFT SUPERSYMMETRY BREAKING MASSES AND mu PARAMETER FROM DYNAMICAL REARRANGEMENT OF EXOTIC U(1) SYMMETRIES"},{"@value":"SOFT SUPERSYMMETRY BREAKING MASSES AND μ PARAMETER FROM DYNAMICAL REARRANGEMENT OF EXOTIC <font>U</font>(1) SYMMETRIES"}]},{"@id":"https://cir.nii.ac.jp/crid/1050856995323665152","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Comprehensive analysis of Yukawa hierarchies on T2/Z(N) with magnetic fluxes"},{"@value":"Comprehensive analysis of Yukawa hierarchies on<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>T</mml:mi><mml:mn>2</mml:mn></mml:msup><mml:mo stretchy=\"false\">/</mml:mo><mml:msub><mml:mi>Z</mml:mi><mml:mi>N</mml:mi></mml:msub></mml:math>with magnetic fluxes"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235008959616","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Flavor symmetry breaking and vacuum alignment on orbifolds"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004236162476544","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"μ PARAMETER FROM DYNAMICAL REARRANGEMENT OF U(1) AND θ PARAMETER"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706096388224","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Topological solitons in the supersymmetric Skyrme model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706111594752","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Impacts of non-geometric moduli on effective theory of 5D supergravity"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285706113518720","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Vortices and monopoles in mass-deformed SO and USp gauge theories"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184963480576","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Neutrino masses and mixing from<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>S</mml:mi><mml:mn>4</mml:mn></mml:msub></mml:math>flavor twisting"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848656054690304","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Enhanced Higgs mass in Compact Supersymmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659943039872","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Compact supersymmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659950094976","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Implications of the 750 GeV diphoton excess in gaugino mediation"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659956087424","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Orbifold family unification using vectorlike representation on six dimensions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360857593802937216","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Target space duality of non-supersymmetric string theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861707114915072","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Aiming for unification of Lμ − Lτ and the standard model gauge group"}]},{"@id":"https://cir.nii.ac.jp/crid/1360869854360646912","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Computation of the index on orbifold from the Atiyah-Segal-Singer fixed point theorem"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001204155692544","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Matter Representations and Gauge Symmetry Breaking via Compactified Space."}]},{"@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/2050870367085247744","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Notes on a vanishing cosmological constant without Bose-Fermi cancellation"}]},{"@id":"https://cir.nii.ac.jp/crid/2051151842055151744","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Exponentially suppressed cosmological constant with enhanced gauge symmetry in heterotic interpolating models"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1016/0370-2693(79)90425-8"},{"@type":"CROSSREF","@value":"10.1007/jhep02(2016)184_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1093/ptep/pty095_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1103/physrevd.78.115006_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1103/physrevd.84.025018_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1103/physrevd.88.055016_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1142/s0217751x11054516_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1142/s0217751x12500236_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1142/s0217751x13500553_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1007/jhep01(2014)065_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1007/jhep01(2017)014_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1007/jhep11(2013)090_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1007/jhep12(2011)017_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1103/physrevd.81.075011_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1103/physrevd.94.035031_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1016/j.nuclphysb.2014.11.022_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptac061_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1103/physrevd.83.033004_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1016/j.nuclphysb.2015.03.004_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1143/ptp.102.407_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1007/jhep04(2016)025_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1007/jhep07(2015)022_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1103/physrevd.86.115014_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1103/physrevd.93.055025_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1103/physrevd.98.035039_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1016/j.nuclphysb.2022.115667_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1007/jhep07(2022)011_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1016/j.nuclphysb.2020.115111_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1103/physrevd.110.105013_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptz123_references_DOI_CC9uOfodyazrVjipsNHduURG5bM"}]}