{"@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/1360568469921484928.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevd.100.055030"}},{"identifier":{"@type":"URI","@value":"https://link.aps.org/article/10.1103/PhysRevD.100.055030"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.100.055030/fulltext"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@value":"Complete vectorlike fourth family and new \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><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:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>\n for muon anomalies"}],"description":[{"notation":[{"@value":"We consider the Standard Model (SM) with the addition of a $\\mathrm{U}(1{)}^{\\ensuremath{'}}$ gauge symmetry and a complete fourth family of quarks and leptons which are vectorlike with respect to the full $\\mathrm{SU}(3{)}_{\\mathrm{C}}\\ifmmode\\times\\else\\texttimes\\fi{}\\mathrm{SU}(2{)}_{\\mathrm{L}}\\ifmmode\\times\\else\\texttimes\\fi{}\\mathrm{U}(1{)}_{\\mathrm{Y}}\\ifmmode\\times\\else\\texttimes\\fi{}\\mathrm{U}(1{)}^{\\ensuremath{'}}$ gauge symmetry. The model provides a unified explanation of experimental anomalies in $(g\\ensuremath{-}2{)}_{\\ensuremath{\\mu}}$ as well as $b\\ensuremath{\\rightarrow}s{\\ensuremath{\\ell}}^{+}{\\ensuremath{\\ell}}^{\\ensuremath{-}}$ decays. We find good fits to the deviations from the SM, while at the same time fitting all other SM observables. The model includes a new ${Z}^{\\ensuremath{'}}$ gauge boson, a $\\mathrm{U}(1{)}^{\\ensuremath{'}}$-breaking scalar, and vectorlike leptons all with mass of order a few hundred giga-electron-volts. It is consistent with all currently released high energy experimental data; however, it appears imminently testable with well-designed future searches. Also, precision flavor experiments, especially more accurate direct determinations of Cabibbo-Kobayashi-Maskawa matrix elements, would allow probing the best fit points."}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1420845751157888640","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"00814667"},{"@type":"NRID","@value":"1000000814667"}],"foaf:name":[{"@value":"Junichiro Kawamura"}]},{"@id":"https://cir.nii.ac.jp/crid/1380568469921484416","@type":"Researcher","foaf:name":[{"@value":"Stuart Raby"}]},{"@id":"https://cir.nii.ac.jp/crid/1380568469921484928","@type":"Researcher","foaf:name":[{"@value":"Andreas Trautner"}]}],"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":"2019-09-18","prism:volume":"100","prism:number":"5"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["https://creativecommons.org/licenses/by/4.0/"],"url":[{"@id":"https://link.aps.org/article/10.1103/PhysRevD.100.055030"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.100.055030/fulltext"}],"createdAt":"2019-09-18","modifiedAt":"2019-09-18","project":[{"@id":"https://cir.nii.ac.jp/crid/1040000782003458048","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"18K13534"},{"@type":"JGN","@value":"JP18K13534"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-18K13534/"}],"notation":[{"@language":"ja","@value":"ニュートリノ質量を説明する最小超対称標準模型の構築"},{"@language":"en","@value":"Minimal supersymmetric standard models for neutrino masses"}]}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360002217829224064","@type":"Article","resourceType":"学術雑誌論文(journal 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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> TeV</mml:mtext></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361975844805506560","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Complete vectorlike fourth family with \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><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:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>\n: A global analysis"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981468379043968","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Measurement of the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>B</mml:mi><mml:mo stretchy=\"false\">→</mml:mo><mml:msub><mml:mrow><mml:mi>X</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub><mml:msup><mml:mrow><mml:mo>ℓ</mml:mo></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mrow><mml:mo>ℓ</mml:mo></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>Branching Fraction and Search for Direct<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>C</mml:mi><mml:mi>P</mml:mi></mml:math>Violation from a Sum of Exclusive Final States"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981468497083776","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Test of Lepton Universality Using<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>B</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mi>K</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mo>ℓ</mml:mo><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mo>ℓ</mml:mo><mml:mo>−</mml:mo></mml:msup></mml:math>Decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981468784525824","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>B</mml:mi><mml:mo>→</mml:mo><mml:msup><mml:mi>K</mml:mi><mml:mrow><mml:mo mathvariant=\"bold\" stretchy=\"false\">(</mml:mo><mml:mo>*</mml:mo><mml:mo mathvariant=\"bold\" stretchy=\"false\">)</mml:mo></mml:mrow></mml:msup><mml:mi>ν</mml:mi><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math>and invisible quarkonium decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981469784225920","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Status of the \n                $$B\\rightarrow K^*\\mu ^+\\mu ^-$$\n                \n                    \n                                    \n                        \n                            B\n                            →\n                            \n                                K\n                                ∗\n                            \n                            \n                                μ\n                                +\n                            \n                            \n                                μ\n                                -\n                            \n                        \n                    \n                \n             anomaly after Moriond 2017"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470109891200","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Model-Independent Bounds on Kinetic Mixing"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470513550464","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for pair production of heavy vector-like quarks decaying to high-p T W bosons and b quarks in the lepton-plus-jets final state in pp collisions at s = 13 $$ \\sqrt{s}=13 $$ TeV with the ATLAS detector"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981471356863744","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"B→Xse+e− in the six-quark model"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262943701550720","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msup><mml:mo>−</mml:mo><mml:msup><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo accent=\"true\" 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Rev. D \n<b>93</b>\n, 055045 (2016)]"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544420057848192","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Bs mixing observables and |Vtd/Vts| from sum rules"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544420742693376","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"The anatomy of Z ′ and Z with flavour changing neutral currents in the flavour precision era"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544420863329024","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Muon anomalous magnetic moment: A harbinger for “new physics”"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825893941073536","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"B-physics from Nf = 2 tmQCD: the Standard Model and 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mathvariant=\"italic\">e</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant=\"normal\">−</mml:mi></mml:mrow></mml:msup></mml:mrow></mml:math>beyond leading logarithms in the naive dimensional regularization and ’t Hooft–Veltman schemes"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825894419973632","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"R(K(⁎)) from dark matter exchange"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825894759108224","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"g μ − 2 from Vector-like leptons in warped space"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825895163344512","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Simple interpretations of lepton anomalies in the lepton-specific inert two-Higgs-doublet model"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825896042280448","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Limits on 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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:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>\n behind \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>b</mml:mi><mml:mo stretchy=\"false\">→</mml:mo><mml:mi>s</mml:mi><mml:mo>ℓ</mml:mo><mml:mo>ℓ</mml:mo></mml:mrow></mml:math>\n anomalies at the LHC"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388843763480320","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Updated \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>B</mml:mi><mml:mi>s</mml:mi></mml:msub></mml:math>\n-mixing constraints on new physics models for \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>b</mml:mi><mml:mo stretchy=\"false\">→</mml:mo><mml:mi>s</mml:mi><mml:msup><mml:mrow><mml:mo>ℓ</mml:mo></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mrow><mml:mo>ℓ</mml:mo></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>\n anomalies"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388844116026240","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Differential branching fractions and isospin asymmetries of B → K (*) μ + μ − decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388844730831872","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Master formulae for ΔF=2 NLO-QCD factors in the Standard Model and beyond"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388844784463104","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Interpreting hints for lepton flavor universality 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stretchy=\"false\">→</mml:mo><mml:msup><mml:mrow><mml:mo>ℓ</mml:mo></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mrow><mml:mo>ℓ</mml:mo></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>in the Standard Model with Reduced Theoretical Uncertainty"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388846201005312","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Neutrino trident scattering at near detectors"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670318372136576","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Patterns of New Physics in b → sℓ+ℓ− transitions in the light of recent data"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670318710285184","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Vectorlike leptons: Muon \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>g</mml:mi><mml:mo>−</mml:mo><mml:mn>2</mml:mn></mml:math>\n anomaly, lepton flavor violation, Higgs boson decays, and lepton nonuniversality"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670319253743744","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Flavourful Z\n                            ′ models for \n\n\n                                    \n\nR\n\nK\n\n∗\n\n\n\n\n\n$$ {R}_{K^{\\left(\\ast \\right)}} $$"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670319687071360","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"UFO – The Universal FeynRules Output"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670320085602688","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for Lepton-Universality Violation in \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>B</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mi>K</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mo>ℓ</mml:mo><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mo>ℓ</mml:mo><mml:mo>−</mml:mo></mml:msup></mml:math>\n Decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670320666282880","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"A simple model for explaining muon-related anomalies and dark matter"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670320945721600","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Vector-like leptons: Higgs decays and collider phenomenology"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670321213190912","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>B</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mi>K</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>τ</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>τ</mml:mi><mml:mo>−</mml:mo></mml:msup></mml:math>\n at the \n<i>BaBar</i>\n Experiment"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670321232811392","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Vectorlike leptons at the Large Hadron Collider"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951793658281472","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951794643450752","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Angular analysis of B0 d → K∗μ+μ− decays in pp collisions at $$ \\sqrt{s}=8 $$ TeV with the ATLAS detector"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951794686092416","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Vectorlike chiral fourth family to explain muon anomalies"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951795743982848","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Towards the discovery of new physics with lepton-universality ratios of \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>b</mml:mi><mml:mo stretchy=\"false\">→</mml:mo><mml:mi>s</mml:mi><mml:mo>ℓ</mml:mo><mml:mo>ℓ</mml:mo></mml:math>\n decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233268637541760","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Quark flavor transitions in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi>L</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:msub><mml:mo>−</mml:mo><mml:msub><mml:mrow><mml:mi>L</mml:mi></mml:mrow><mml:mrow><mml:mi>τ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>models"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233268709644672","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Explanation of the muon<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>g</mml:mi><mml:mo mathvariant=\"bold\">−</mml:mo><mml:mn>2</mml:mn></mml:math>anomaly with vectorlike leptons and its implications for Higgs decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233268801827328","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"B\n                            \n                                s\n                             → μ\n                            +\n                            μ\n                            − as current and future probe of new physics"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233269848385408","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Neutrino trident production at the intensity frontier"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233269918215296","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<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>models for the LHCb and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>g</mml:mi><mml:mo>−</mml:mo><mml:mn>2</mml:mn></mml:math>muon anomalies"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233270859634944","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Explaining<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>h</mml:mi><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mo>±</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mrow><mml:mi>τ</mml:mi></mml:mrow><mml:mrow><mml:mo>∓</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>,<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>B</mml:mi><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mi>K</mml:mi><mml:mo>*</mml:mo></mml:msup><mml:msup><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mrow><mml:mi>μ</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:mi>B</mml:mi><mml:mo stretchy=\"false\">→</mml:mo><mml:mi>K</mml:mi><mml:msup><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mo>/</mml:mo><mml:mi>B</mml:mi><mml:mo stretchy=\"false\">→</mml:mo><mml:mi>K</mml:mi><mml:msup><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><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>in a Two-Higgs-Doublet Model with Gauged<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi>L</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:msub><mml:mtext>−</mml:mtext><mml:msub><mml:mrow><mml:mi>L</mml:mi></mml:mrow><mml:mrow><mml:mi>τ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233270951192576","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>B</mml:mi><mml:mo>→</mml:mo><mml:msup><mml:mi>h</mml:mi><mml:mrow><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>*</mml:mo><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:msup><mml:mi>ν</mml:mi><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math>with the full Belle<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>Υ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>4</mml:mn><mml:mi>S</mml:mi><mml:mo stretchy=\"false\">)</mml:mo></mml:math>data sample"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233271041976960","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Explaining the \n                $$R_K$$\n                \n                    \n                        \n                            R\n                            K\n                        \n                    \n                \n             and \n                $$R_{K^*}$$\n                \n                    \n                        \n                            R\n                            \n                                K\n                                ∗\n                            \n                        \n                    \n                \n             anomalies"}]},{"@id":"https://cir.nii.ac.jp/crid/1524232504846267648","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Effects of Superheavy Quarks and Leptons in Low-Energy Weak 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