{"@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/1360002217829072256.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevd.95.115040"}},{"identifier":{"@type":"URI","@value":"http://link.aps.org/article/10.1103/PhysRevD.95.115040"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.95.115040/fulltext"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.1702.08666"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@value":"LHCb anomaly and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>B</mml:mi></mml:math>\n physics in flavored \n<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:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>\n models with flavored Higgs doublets"}],"description":[{"notation":[{"@value":"We study an extended Standard Model with a gauged U(1)$^{\\prime}$ flavor symmetry, motivated not only by the fermion mass hierarchy but also by the excesses in $B \\to K^{(*)} l l$ reported by the LHCb collaborations. The U(1)$^{\\prime}$ charges are assigned to quarks and leptons in a flavor-dependent manner, and flavored Higgs doublets are also introduced in order to detail the Yukawa couplings at the renormalizable level. Then, the fermion mass hierarchy is realized by the vacuum alignment of the Higgs doublets. In this model, flavor-changing currents involving the gauge boson of U(1)$^{\\prime}$ and the scalars generated by the Higgs doublets are predicted and the observables in the $B \\to K^{(*)} l l$ process possibly deviate from the Standard Model predictions. We study the possibility that these new flavor-changing interactions can explain the excesses in the $B \\to K^{(*)} l l$ process, and we derive some predictions for the other flavor-violating processes based on the analysis. We specifically investigate the $��F=2$ processes and the other $B$ decays: e.g., $B \\to X_s ��$ and $B \\to D^{(*)} ����$, where the deviations are reported by the Belle and $BABAR$ collaborations."}]},{"notation":[{"@value":"28 pages, 5 figures, v2: texts and figures are improved"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380566395998324226","@type":"Researcher","foaf:name":[{"@value":"P. Ko"}]},{"@id":"https://cir.nii.ac.jp/crid/1380566395998324227","@type":"Researcher","foaf:name":[{"@value":"Yuji Omura"}]},{"@id":"https://cir.nii.ac.jp/crid/1380566395998324225","@type":"Researcher","foaf:name":[{"@value":"Yoshihiro Shigekami"}]},{"@id":"https://cir.nii.ac.jp/crid/1380566395998324224","@type":"Researcher","foaf:name":[{"@value":"Chaehyun Yu"}]}],"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":"2017-06-30","prism:volume":"95","prism:number":"11","prism:startingPage":"115040"},"reviewed":"false","dc:rights":["http://link.aps.org/licenses/aps-default-license"],"url":[{"@id":"http://link.aps.org/article/10.1103/PhysRevD.95.115040"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.95.115040/fulltext"}],"createdAt":"2017-06-30","modifiedAt":"2017-06-30","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-%20Experiment%20(hep-ex)","dc:title":"High Energy Physics - Experiment (hep-ex)"},{"@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"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Experiment","dc:title":"High Energy Physics - Experiment"}],"project":[{"@id":"https://cir.nii.ac.jp/crid/1040000781905464960","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"16J08299"},{"@type":"JGN","@value":"JP16J08299"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-16J08299/"}],"notation":[{"@language":"ja","@value":"超対称大統一理論を用いた模型の構築"}]},{"@id":"https://cir.nii.ac.jp/crid/1040000781958729088","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"17H05404"},{"@type":"JGN","@value":"JP17H05404"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PUBLICLY-17H05404/"}],"notation":[{"@language":"ja","@value":"フレーバー物理による暗黒物質と真空構造の解明"},{"@language":"en","@value":"Investigation of dark matter and vacuum structure via flavor physics"}]}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050001335851866880","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Review of lattice results concerning low-energy particle physics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360002217826330752","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Tau longitudinal polarization in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mover accent=\"true\"><mml:mi>B</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mo>→</mml:mo><mml:mi>D</mml:mi><mml:mi>τ</mml:mi><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math>and its role in the search for the charged Higgs boson"}]},{"@id":"https://cir.nii.ac.jp/crid/1360002217829224064","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Interplay between the \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:mi>l</mml:mi><mml:mi>l</mml:mi></mml:math>\n anomalies and dark matter physics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235015540864","@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>C</mml:mi><mml:mi>P</mml:mi></mml:math>violation in<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>D</mml:mi><mml:mi>τ</mml:mi><mml:msub><mml:mi>ν</mml:mi><mml:mi>τ</mml:mi></mml:msub></mml:math>using multipion tau decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011143616657536","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"A closer look at the R D and R D* anomalies"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011143877331200","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"ΔMs/ΔMd, sin2β and the angle γ in the presence of new ΔF=2 operators"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011144265758720","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Explaining<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>B</mml:mi><mml:mo>→</mml:mo><mml:mi>D</mml:mi><mml:mi>τ</mml:mi><mml:mi>ν</mml:mi></mml:math>,<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>D</mml:mi><mml:mo>*</mml:mo></mml:msup><mml:mi>τ</mml:mi><mml:mi>ν</mml:mi></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>B</mml:mi><mml:mo>→</mml:mo><mml:mi>τ</mml:mi><mml:mi>ν</mml:mi></mml:math>in a two Higgs doublet model of type III"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011145521580928","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Angular analysis of the B\n                            0 → K\n                            *0\n                            μ\n                            +\n                            μ\n                            − decay using 3 fb−1 of integrated luminosity"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011145909163648","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Azimuthal<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:mrow><mml:mi>D</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:msub><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mo accent=\"true\" stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mi>τ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>angular distribution with tensor operators"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011146537616256","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Two Higgs doublet models for the LHC Higgs boson data at s $$ \\sqrt{s} $$ = 7 and 8 TeV"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011146605385984","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Tau properties in \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>D</mml:mi><mml:mi>τ</mml:mi><mml:mi>ν</mml:mi></mml:math>\n from visible final-state kinematics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360283692432037248","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Review of Particle Physics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360283692804245760","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Testing leptoquark models in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mover accent=\"true\"><mml:mi>B</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mo>→</mml:mo><mml:msup><mml:mi>D</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>τ</mml:mi><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360283692804878976","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Probing new physics with<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>q</mml:mi><mml:mn>2</mml:mn></mml:msup></mml:math>distributions in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>B</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover><mml:mo>→</mml:mo><mml:msup><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>*</mml:mo><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:msup><mml:mi>τ</mml:mi><mml:mover accent=\"true\"><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292618644040448","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Leptoquark flavor patterns & B decay anomalies"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292619049287680","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"B-decay anomalies in a composite leptoquark model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292619201568640","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Flavor-phenomenology of two-Higgs-doublet models with generic Yukawa structure"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292620293064704","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Flavor constraints on the Two Higgs Doublet Models of Z 2 symmetric and aligned types"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292620455052800","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"On the anomalies in the latest LHCb data"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292620517186176","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Two Higgs doublet model predictions for<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mrow><mml:mover><mml:mrow><mml:mi>B</mml:mi></mml:mrow><mml:mrow><mml:mi>¯</mml:mi></mml:mrow></mml:mover></mml:mrow></mml:mrow><mml:mo>→</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>X</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mi>γ</mml:mi></mml:math>in NLO QCD"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292620734108544","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Implications of Lepton Flavor Universality Violations in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>B</mml:mi></mml:math>Decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1360565167781737088","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Measurement of the branching ratio of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>B</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>*</mml:mo><mml:mo stretchy=\"false\">)</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:msub><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mi>τ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>relative to<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mover accent=\"true\"><mml:mi>B</mml:mi><mml:mo stretchy=\"false\">¯</mml:mo></mml:mover><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mi>D</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:msup><mml:mo>ℓ</mml:mo><mml:mo>−</mml:mo></mml:msup><mml:msub><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo stretchy=\"false\">¯</mml:mo></mml:mover><mml:mo>ℓ</mml:mo></mml:msub></mml:math>decays with hadronic tagging at Belle"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567181090496768","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for flavour-changing neutral current top quark decays t → Hq in pp collisions at s = 8 $$ \\sqrt{s}=8 $$ TeV with the ATLAS detector"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184981142272","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Test of the \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>R</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:msup><mml:mi>D</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:mo stretchy=\"false\">)</mml:mo></mml:math>\n anomaly at the LHC"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574093505601536","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>B</mml:mi><mml:mo>→</mml:mo><mml:mi>D</mml:mi><mml:mi>τ</mml:mi><mml:mi>ν</mml:mi></mml:math>branching ratios: Opportunity for lattice QCD and hadron colliders"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574093894763648","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"A comprehensive analysis of hadronic<i>b</i>→<i>s</i>transitions in a family non-universal<i>Z</i>′ model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574094193947520","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Explaining \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:msup><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>*</mml:mo><mml:mo stretchy=\"false\">)</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: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 anomaly by radiatively induced coupling in \n<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:msub><mml:mrow><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow><mml:mrow><mml:mi>μ</mml:mi><mml:mo>−</mml:mo><mml:mi>τ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>\n gauge symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574095173005184","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Impact of family-non-universal $$Z^\\prime $$ Z ′ boson on pure annihilation $$B_s \\rightarrow \\pi ^+ \\pi ^-$$ B s → π + π - and $$B_d \\rightarrow K^+ K^-$$ B d → K + K - decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574095855433088","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for minimal supersymmetric standard model Higgs Bosons H / A and for a $$Z^{\\prime }$$ Z ′ boson in the $$\\tau \\tau $$ τ τ final state produced in pp collisions at $$\\sqrt{s}= 13$$ s = 13 TeV with the ATLAS detector"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574096039239040","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Measurement of Form-Factor-Independent Observables in the Decay<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>B</mml:mi><mml:mn>0</mml:mn></mml:msup><mml:mo>→</mml:mo><mml:msup><mml:mi>K</mml:mi><mml:mrow><mml:mo>*</mml:mo><mml:mn>0</mml:mn></mml:mrow></mml:msup><mml:msup><mml:mi>μ</mml:mi><mml:mo mathvariant=\"bold\">+</mml:mo></mml:msup><mml:msup><mml:mi>μ</mml:mi><mml:mo mathvariant=\"bold\">−</mml:mo></mml:msup></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574096148040576","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"B → K*ℓ + ℓ −, Kℓ + ℓ − decays in a family non-universal Z′ model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574096322388736","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Addendum to “Two Higgs doublet model predictions for<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mrow><mml:mover><mml:mrow><mml:mi>B</mml:mi></mml:mrow><mml:mrow><mml:mi>¯</mml:mi></mml:mrow></mml:mover></mml:mrow></mml:mrow><mml:mo>→</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mi>X</mml:mi></mml:mrow><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mi>γ</mml:mi></mml:math>in NLO QCD”"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574096429735680","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Non-abelian gauge extensions for B-decay anomalies"}]},{"@id":"https://cir.nii.ac.jp/crid/1360846642757377792","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"New physics in the weak interaction of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mover accent=\"true\"><mml:mi>B</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mo>→</mml:mo><mml:msup><mml:mi>D</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>τ</mml:mi><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360846642767571200","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Effective Field Theory Approach to<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:msup><mml:mo>ℓ</mml:mo><mml:mrow><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>′</mml:mo><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:msup></mml:math>,<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:msup><mml:mi>K</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 stretchy=\"false\">¯</mml:mo></mml:mover></mml:math>and<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:msup><mml:mi>D</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>τ</mml:mi><mml:mi>ν</mml:mi></mml:math>with Third Generation Couplings"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855569446333824","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Minimal Leptoquark Explanation for the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>R</mml:mi><mml:msup><mml:mi>D</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:msub></mml:math>,<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>R</mml:mi><mml:mi>K</mml:mi></mml:msub></mml:math>, and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>g</mml:mi><mml:mo>−</mml:mo><mml:mn>2</mml:mn><mml:msub><mml:mo stretchy=\"false\">)</mml:mo><mml:mi>μ</mml:mi></mml:msub></mml:math>Anomalies"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855569706257664","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Higgs phenomenology in Type-I 2HDM with U(1) H Higgs gauge symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855569969166720","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Leptoquark model to explain the \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>B</mml:mi></mml:mrow></mml:math>\n-physics anomalies, \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>K</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>\n and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>D</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855570301421440","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Understanding the<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:mo>*</mml:mo></mml:msup><mml:msup><mml:mi>μ</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>μ</mml:mi><mml:mo>−</mml:mo></mml:msup></mml:math>anomaly"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855571396030208","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"B ¯ → D ∗ τ ν ¯ $$ \\overline{B}\\to {D}^{\\left(\\ast \\right)}\\tau \\overline{\\nu} $$ excesses in ALRSM constrained from B, D decays and D 0 − D ¯ 0 $$ {D}^0-{\\overline{D}}^0 $$ mixing"}]},{"@id":"https://cir.nii.ac.jp/crid/1360857593726608000","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Higgs flavor phenomenology in a supersymmetric left-right model with parity"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137043962818432","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Erratum:<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>D</mml:mi><mml:mi>l</mml:mi><mml:mi>ν</mml:mi></mml:mrow></mml:math>form factors at nonzero recoil and extraction of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mo stretchy=\"false\">|</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>b</mml:mi></mml:mrow></mml:msub><mml:mo stretchy=\"false\">|</mml:mo></mml:mrow></mml:math>[Phys. Rev. D<b>92</b>, 054510 (2015)]"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137044905889408","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Family non-universal Z′ effects on $ {\\bar B_q} - {B_q} $ mixing, B → X s μ + μ − and B s → μ + μ − decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137045524305152","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Consequences of R-parity violating interactions for anomalies in $${\\bar{B}}\\rightarrow D^{(*)} \\tau {\\bar{\\nu }}$$ B ¯ → D ( ∗ ) τ ν ¯ and $$b\\rightarrow s \\mu ^+\\mu ^-$$ b → s μ + μ -"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137045564547840","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Anomalies in B-decays and U(2) flavor symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137045920246400","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Towards a unified explanation of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>*</mml:mo><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:msub></mml:mrow></mml:math>,<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>K</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>g</mml:mi><mml:mo>−</mml:mo><mml:mn>2</mml:mn><mml:msub><mml:mrow><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>anomalies in a left-right model with leptoquarks"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137046122946688","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Addressing the LHC flavor anomalies with horizontal gauge symmetries"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137046324566912","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Dark matter and dark force in the type-I inert 2HDM with local U(1) H gauge symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418518761687168","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"New physics in the kinematic distributions of \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mover accent=\"true\"><mml:mi>B</mml:mi><mml:mo stretchy=\"true\">¯</mml:mo></mml:mover><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mi>D</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:msup><mml:mi>τ</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mo stretchy=\"false\">(</mml:mo><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mo>ℓ</mml:mo><mml:mo>−</mml:mo></mml:msup><mml:msub><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo stretchy=\"true\">¯</mml:mo></mml:mover><mml:mo>ℓ</mml:mo></mml:msub><mml:msub><mml:mi>ν</mml:mi><mml:mi>τ</mml:mi></mml:msub><mml:mo stretchy=\"false\">)</mml:mo><mml:msub><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo stretchy=\"true\">¯</mml:mo></mml:mover><mml:mi>τ</mml:mi></mml:msub></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418519046182400","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"LHC constraints and prospects for<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>S</mml:mi><mml:mn>1</mml:mn></mml:msub></mml:math>scalar leptoquark explaining the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mover accent=\"true\"><mml:mi>B</mml:mi><mml:mo stretchy=\"true\">¯</mml:mo></mml:mover><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mi>D</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>τ</mml:mi><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo stretchy=\"true\">¯</mml:mo></mml:mover></mml:math>anomaly"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418519657899904","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"B → D\n              (*)\n              τν and B → τν in chiral U(1)′ models with flavored multi Higgs doublets"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520056001408","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Chiral U(1) flavor models and flavored Higgs doublets: the top FB asymmetry and the W jj"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418521052600320","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Scalar contributions to b→c(u)τν transitions"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418521314235392","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Revisiting Lepton Flavor Universality in \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>B</mml:mi></mml:math>\n Decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418521446317312","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Lepton universality violation with lepton flavor conservation in B-meson decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699993839593984","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<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>D</mml:mi><mml:mo>ℓ</mml:mo><mml:mi>ν</mml:mi></mml:math>form factors at nonzero recoil and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mo stretchy=\"false\">|</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>b</mml:mi></mml:mrow></mml:msub><mml:mo stretchy=\"false\">|</mml:mo></mml:mrow></mml:math>from<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mn>2</mml:mn><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:math>-flavor lattice QCD"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699994304978816","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Search for top quark decays via Higgs-boson-mediated flavor-changing neutral currents in pp collisions at \n                      s\n                    =\n                    8\n                $$ \\sqrt{s}=8 $$\n               TeV"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699994755476864","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Phenomenology of an SU(2) × SU(2) × U(1) model with lepton-flavour non-universality"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995759546624","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Higgs and dark matter physics in the type-II two-Higgs-doublet model inspired by E 6 GUT"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699996437280128","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Measurement of the Ratio of Branching Fractions<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi mathvariant=\"script\">B</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:msup><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>B</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msup><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo>*</mml:mo><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:msub><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mi>τ</mml:mi></mml:mrow></mml:msub><mml:mo stretchy=\"false\">)</mml:mo><mml:mo stretchy=\"false\">/</mml:mo><mml:mi mathvariant=\"script\">B</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:msup><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>B</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msup><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo>*</mml:mo><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:msub><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:msub><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981468465997312","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Anomalous enhancement observed in<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>D</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>τ</mml:mi><mml:msub><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mi>τ</mml:mi></mml:msub></mml:math>decays"}]},{"@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/1361981470109891200","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Model-Independent Bounds on Kinetic Mixing"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470302699264","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"$ \\overline{B}\\ \\to {X_s}\\gamma $ in the Two Higgs Doublet Model up to next-to-next-to-leading order in QCD"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470853587328","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Explaining the \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mi>K</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>\n and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mi>D</mml:mi></mml:mrow><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:mrow></mml:msub></mml:mrow></mml:math>\n anomalies with vector leptoquarks"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470998262656","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:msubsup><mml:mi>B</mml:mi><mml:mi>s</mml:mi><mml:mn>0</mml:mn></mml:msubsup><mml:mtext>–</mml:mtext><mml:msubsup><mml:mover accent=\"true\"><mml:mi>B</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mi>s</mml:mi><mml:mn>0</mml:mn></mml:msubsup></mml:math> mixing and <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si2.gif\" overflow=\"scroll\"><mml:mi>B</mml:mi><mml:mo>→</mml:mo><mml:mi>π</mml:mi><mml:mi>K</mml:mi></mml:math> decays in stringy leptophobic <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si3.gif\" overflow=\"scroll\"><mml:msup><mml:mi>Z</mml:mi><mml:mo>′</mml:mo></mml:msup></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981471466256768","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>B</mml:mi></mml:math>decays with<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>τ</mml:mi></mml:math>leptons in nonuniversal left-right models"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262943641931264","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Sensitivity to charged scalars in B → D (*) τν τ and B → τν τ decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262945092134016","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Minimally flavored colored scalar in $ \\overline{B}\\to {D^{{\\left( * \\right)}}}\\tau \\overline{\\nu} $ and the mass matrices constraints"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262945301095552","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<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>D</mml:mi><mml:mi>l</mml:mi><mml:mi>ν</mml:mi></mml:math>form factors at nonzero recoil and extraction of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mo stretchy=\"false\">|</mml:mo><mml:msub><mml:mrow><mml:mi>V</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>b</mml:mi></mml:mrow></mml:msub><mml:mo stretchy=\"false\">|</mml:mo></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262945676587008","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Hierarchy of quark masses, cabibbo angles and CP violation"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262946023043840","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Diagnosing new physics in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>b</mml:mi><mml:mo>→</mml:mo><mml:mi>c</mml:mi><mml:mi>τ</mml:mi><mml:msub><mml:mi>ν</mml:mi><mml:mi>τ</mml:mi></mml:msub></mml:math>decays in the light of the recent<i>BABAR</i>result"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544419300693120","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Top A FB at the Tevatron vs. charge asymmetry at the LHC in chiral U(1) flavor models with flavored Higgs doublets"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544420123595648","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Top forward-backward asymmetry and the CDF<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>W</mml:mi><mml:mi>j</mml:mi><mml:mi>j</mml:mi></mml:math>excess in leptophobic<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>U</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>1</mml:mn><mml:msup><mml:mo stretchy=\"false\">)</mml:mo><mml:mo>′</mml:mo></mml:msup></mml:math>flavor models"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825893794917120","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Perturbed Lepton-Specific Two-Higgs-Doublet Model Facing Experimental Hints for Physics beyond the Standard Model"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825895848466304","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Sterile neutrinos in leptonic and semileptonic decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107369261454720","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Evidence for an Excess of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mover accent=\"true\"><mml:mi>B</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mo>→</mml:mo><mml:msup><mml:mi>D</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:msup><mml:mi>τ</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:msub><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mi>τ</mml:mi></mml:msub></mml:math>Decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107369417405952","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"$ B_s^0 - \\overline B_s^0 $ mixing in a family non-universal Z′ model revisited"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107370913894656","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Revisiting the one leptoquark solution to the R(D (∗)) anomalies and its phenomenological implications"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107371095411712","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"LHCb anomalies from a natural perspective"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107371272556032","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"New physics in the visible final states of B → D(∗) τν"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388843499503616","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Updated Next-to-Next-to-Leading-Order QCD Predictions for the Weak Radiative \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>B</mml:mi></mml:mrow></mml:math>\n-Meson Decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388843825230336","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Predictions for lepton flavor universality violation in rare B decays in models with gauged<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>L</mml:mi><mml:mi>μ</mml:mi></mml:msub><mml:mo>−</mml:mo><mml:msub><mml:mi>L</mml:mi><mml:mi>τ</mml:mi></mml:msub></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388844640243328","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Scalar doublet models confront<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>τ</mml:mi></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>b</mml:mi></mml:math>anomalies"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670318710180224","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Exploring top quark FCNC within 2HDM type III in association with flavor physics"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670319230805888","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Simultaneous explanation of the R K and R ( D (⁎) ) puzzles"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670320565845120","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Probing new physics in \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>B</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"true\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msup><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>*</mml:mo><mml:mo stretchy=\"false\">)</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:msub><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"true\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mi>τ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>\n using the longitudinal, transverse, and normal polarization components of the tau lepton"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951793236243712","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<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>D</mml:mi><mml:mo>*</mml:mo></mml:msup><mml:mi>τ</mml:mi><mml:msub><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mi>τ</mml:mi></mml:msub></mml:math>sensitivity to new physics"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951794226375552","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Publisher’s Note: Measurement of the Ratio of Branching Fractions<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi mathvariant=\"script\">B</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:msup><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>B</mml:mi></mml:mrow><mml:mrow><mml:mo accent=\"true\" stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msup><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo>*</mml:mo><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:msub><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mo accent=\"true\" stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mi>τ</mml:mi></mml:mrow></mml:msub><mml:mo stretchy=\"false\">)</mml:mo><mml:mo>/</mml:mo><mml:mi mathvariant=\"script\">B</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:msup><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>B</mml:mi></mml:mrow><mml:mrow><mml:mo accent=\"true\" stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msup><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo>*</mml:mo><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:msub><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mo accent=\"true\" stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:msub><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:math>[Phys. Rev. Lett.<b>115</b>, 111803 (2015)]"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951794305299968","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Lifetime of \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msubsup><mml:mi>B</mml:mi><mml:mi>c</mml:mi><mml:mo>−</mml:mo></mml:msubsup></mml:math>\n Mesons Constrains Explanations for Anomalies in \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:msup><mml:mi>D</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>τ</mml:mi><mml:mi>ν</mml:mi></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951794988999680","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Measurement of an excess of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mover accent=\"true\"><mml:mi>B</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mo>→</mml:mo><mml:msup><mml:mi>D</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:msup><mml:mi>τ</mml:mi><mml:mo mathvariant=\"bold\">−</mml:mo></mml:msup><mml:msub><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mi>τ</mml:mi></mml:msub></mml:math>decays and implications for charged Higgs bosons"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951795179026048","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Two U(1)'s and ϵ charge shifts"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951795570548864","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Two-Higgs-doublet type-II and -III models and $$t\\rightarrow c h$$ t → c h at the LHC"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233268370063232","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Flavor models for<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mover accent=\"true\"><mml:mi>B</mml:mi><mml:mo stretchy=\"false\">¯</mml:mo></mml:mover><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mi>D</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>τ</mml:mi><mml:mover accent=\"true\"><mml:mi>ν</mml:mi><mml:mo stretchy=\"false\">¯</mml:mo></mml:mover></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233269283842688","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Probing neutrino and Higgs sectors in $$\\text{ SU(2) }_1 \\times \\text{ SU(2) }_2 \\times \\text{ U(1) }_Y $$ SU(2) 1 × SU(2) 2 × U(1) Y model with lepton-flavor non-universality"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233269391584640","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"On the breaking of lepton flavor universality in B decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233269723544704","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Global analysis of b → sℓℓ anomalies"}]},{"@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/1364233270106745600","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Looking for possible new physics in \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:msup><mml:mi>D</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>τ</mml:mi><mml:msub><mml:mi>ν</mml:mi><mml:mi>τ</mml:mi></mml:msub></mml:math>\n in light of recent data"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233270542173184","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>R</mml:mi><mml:mi>K</mml:mi></mml:msub></mml:math>and future<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>physics beyond the standard model opportunities"}]},{"@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/1364233271140656768","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Simultaneous explanation of the R K and R D * $$ {R}_{D^{\\left(*\\right)}} $$ puzzles: a model analysis"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1103/physrevd.95.115040"},{"@type":"KAKEN","@value":"PRODUCT-21809834"},{"@type":"KAKEN","@value":"PRODUCT-21631116"},{"@type":"OPENAIRE","@value":"doi_dedup___::866101221bac0e51de2dd0cfe83c0a5e"},{"@type":"CROSSREF","@value":"10.1103/physrevd.96.075041_references_DOI_1CEJEuz4QBTEm6kEegm1k4UAADo"},{"@type":"CROSSREF","@value":"10.1103/physrevd.99.075013_references_DOI_1CEJEuz4QBTEm6kEegm1k4UAADo"},{"@type":"CROSSREF","@value":"10.1007/jhep06(2021)125_references_DOI_1CEJEuz4QBTEm6kEegm1k4UAADo"}]}