{"@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/1360285709999053440.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevd.95.035032"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/article/10.1103/PhysRevD.95.035032"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.95.035032/fulltext"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.1612.03378"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@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"}],"description":[{"notation":[{"@value":"In the $SO(5)\\times U(1)$ gauge-Higgs unification (GHU), Kaluza-Klein (KK) excited states of charged and neutral vector bosons, $W^{(1)}$, $W_R^{(1)}$, $Z^{(1)}$, $��^{(1)}$ and $Z_R^{(1)}$, can be observed as $W'$ and $Z'$ signals in collider experiments. In this paper we evaluate the decay rates of the $W'$ and $Z'$, and $s$-channel cross sections mediated by $W'$ and $Z'$ bosons with final states involving the standard model (SM) fermion pair ($\\ell ��$, $\\ell\\bar{\\ell}$, $q\\bar{q}'$), $WH$, $ZH$, $WW$ and $WZ$. $W'$ and $Z'$ resonances appear around 6.0 TeV (8.5 TeV) for $��_H=0.115$ (0.0737) where $��_H$ is the Aharonov-Bohm phase in the fifth dimension in GHU. For decay rates we find $��(W'\\to WH) \\simeq ��(W'\\to WZ)$ ($W'=W^{(1)}$, $W_R^{(1)}$), $��(W^{(1)}\\to WH,WZ) \\sim��(W_R^{(1)}\\to WH,WZ)$, $��(Z^{(1)}\\to ZH) \\simeq\\sum_{Z'=Z^{(1)},��^{(1)}}��(Z'\\to WW)$, and $��(Z_R^{(1)}\\to ZH) \\simeq ��(Z_R^{(1)}\\to WW)$. $W'$ and $Z'$ signals of GHU can be best found at the LHC experiment in the processes $pp\\to W' (Z')+X$ followed by $W'\\to t\\bar{b}$, $WH$, and $Z'\\to e^+ e^-$, $��^+��^-, ZH$. For the lighter $Z'$ ($��_H = 0.115$) case, with forthcoming 30 fb$^{-1}$ data of the 13 TeV LHC experiment we expect about ten $��^+��^-$ events for the invariant mass range 3 to 7 TeV, though the number of the events becomes much smaller when $��_H=0.0737$. In the process with $WZ$ in the final state, it is confirmed that the unitarity is preserved, provided that all KK excited intermediate states are taken into account. Deviation of the $WWZ$ coupling from the SM is very tiny. Exotic partners $t_T^{(1)}$ and $b_Y^{(1)}$ of the top and bottom quarks with electric charge $+5/3$ and $-4/3$ have mass $M_{t_T^{(1)},b_Y^{(1)}}\\simeq 4-5$ TeV, becoming the lightest non-SM particles in GHU which can be singly produced in collider experiments."}]},{"notation":[{"@value":"66 pages, 10 figures, 18 tables (v2) typos corrected, reference added (v3) comments added (v4) match the published version"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380285709999053313","@type":"Researcher","foaf:name":[{"@value":"Shuichiro Funatsu"}]},{"@id":"https://cir.nii.ac.jp/crid/1380285709999053440","@type":"Researcher","foaf:name":[{"@value":"Hisaki Hatanaka"}]},{"@id":"https://cir.nii.ac.jp/crid/1420282801187122304","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"50324744"},{"@type":"NRID","@value":"1000050324744"},{"@type":"CINII_AUTHOR_ID","@value":"DA1913009X"},{"@type":"URI","@value":"https://ci.nii.ac.jp/author/DA1913009X#entity"},{"@type":"URI","@value":"https://viaf.org/viaf/NII%7CDA1913009X"},{"@type":"NRID","@value":"9000351496633"},{"@type":"NRID","@value":"9000351491692"},{"@type":"NRID","@value":"9000006552023"},{"@type":"NRID","@value":"9000003433136"},{"@type":"NRID","@value":"9000003550044"},{"@type":"NRID","@value":"9000006552684"},{"@type":"NRID","@value":"9000010547208"},{"@type":"NRID","@value":"9000003398822"},{"@type":"NRID","@value":"9000364772781"},{"@type":"NRID","@value":"9000002819073"},{"@type":"NRID","@value":"9000006144210"},{"@type":"NRID","@value":"9000017667090"},{"@type":"NRID","@value":"9000006552645"},{"@type":"NRID","@value":"9000402475685"},{"@type":"NRID","@value":"9000258203972"},{"@type":"NRID","@value":"9000008205302"},{"@type":"NRID","@value":"9000397943413"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/read0068751"}],"foaf:name":[{"@value":"Yutaka Hosotani"}]},{"@id":"https://cir.nii.ac.jp/crid/1380285709999053312","@type":"Researcher","foaf:name":[{"@value":"Yuta Orikasa"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"24700010"},{"@type":"EISSN","@value":"24700029"}],"prism:publicationName":[{"@value":"Physical Review D"}],"dc:publisher":[{"@value":"American Physical Society (APS)"}],"prism:publicationDate":"2017-02-27","prism:volume":"95","prism:number":"3","prism:startingPage":"035032"},"reviewed":"false","dc:rights":["http://link.aps.org/licenses/aps-default-license"],"url":[{"@id":"http://link.aps.org/article/10.1103/PhysRevD.95.035032"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.95.035032/fulltext"}],"createdAt":"2017-02-27","modifiedAt":"2017-04-06","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Phenomenology","dc:title":"High Energy Physics - Phenomenology"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Phenomenology%20(hep-ph)","dc:title":"High Energy Physics - Phenomenology (hep-ph)"},{"@id":"https://cir.nii.ac.jp/all?q=FOS:%20Physical%20sciences","dc:title":"FOS: Physical sciences"}],"project":[{"@id":"https://cir.nii.ac.jp/crid/1040000781844546688","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"15K05052"},{"@type":"JGN","@value":"JP15K05052"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-15K05052/"}],"notation":[{"@language":"ja","@value":"自発的対称性の破れ、細谷機構のダイナミックス"},{"@language":"en","@value":"Dynamics of Spontaneous Symmetry Breaking and the Hosotani Mechanism"}]}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050282677610600064","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Search for new phenomena in dijet mass and angular distributions from pp collisions 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unification"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285707420871808","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Distinct signals of the gauge-Higgs unification in e + e − collider experiments"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285709989831424","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Anomalous Higgs interactions in gauge-Higgs unification"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285709992284160","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"LHC signals of the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>SO</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>5</mml:mn><mml:mo stretchy=\"false\">)</mml:mo><mml:mo>×</mml:mo><mml:mi mathvariant=\"normal\">U</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:math>gauge-Higgs unification"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285709996019328","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"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/1360285711139361664","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Gauge-Higgs EW and grand unification"}]},{"@id":"https://cir.nii.ac.jp/crid/1360290617708525312","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Effective potential and universality in GUT-inspired gauge-Higgs 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Rev. D<b>78</b>, 096002 (2008)]"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292620420375296","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for a massive resonance decaying into a Higgs boson and a W or Z boson in hadronic final states in proton-proton collisions at \n                      s\n                    =\n                    8\n                $$ \\sqrt{s}=8 $$\n               TeV"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292621038944640","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Extra-dimensional models on the lattice"}]},{"@id":"https://cir.nii.ac.jp/crid/1360298336550535040","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"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 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LHC"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574093998517376","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for new physics in final states with a lepton and missing transverse energy in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>p</mml:mi><mml:mi>p</mml:mi></mml:math>collisions at the LHC"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574095361984768","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Phenomenology of the Randall-Sundrum Gauge Hierarchy Model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574096431113856","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Dynamics of non-integrable phases and gauge symmetry breaking"}]},{"@id":"https://cir.nii.ac.jp/crid/1360580229799028736","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Bhabha scattering in the 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display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi>W</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mi>W</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi>Z</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mi>Z</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>pair production in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>,<mml:math 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overflow=\"scroll\"><mml:msqrt><mml:mi>s</mml:mi></mml:msqrt><mml:mo>=</mml:mo><mml:mn>8</mml:mn><mml:mtext> </mml:mtext><mml:mtext>TeV</mml:mtext></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361694369828937728","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"CKM matrix and FCNC suppression in \n<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 mathvariant=\"bold\" stretchy=\"false\">(</mml:mo><mml:mn>5</mml:mn><mml:mo mathvariant=\"bold\" stretchy=\"false\">)</mml:mo><mml:mo>×</mml:mo><mml:mi>U</mml:mi><mml:mo mathvariant=\"bold\" stretchy=\"false\">(</mml:mo><mml:mn>1</mml:mn><mml:mo mathvariant=\"bold\" stretchy=\"false\">)</mml:mo><mml:mo>×</mml:mo><mml:mi>S</mml:mi><mml:mi>U</mml:mi><mml:mo mathvariant=\"bold\" stretchy=\"false\">(</mml:mo><mml:mn>3</mml:mn><mml:mo mathvariant=\"bold\" 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