{"@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/1360869854373536256.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevd.111.l011901"}},{"identifier":{"@type":"URI","@value":"https://link.aps.org/article/10.1103/PhysRevD.111.L011901"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.111.L011901/fulltext"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@value":"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: Blinding for data-driven hadronic vacuum polarization"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:p>The KNTW (Keshavarzi-Nomura-Teubner-Wright) data-driven determinations of the hadronic vacuum polarization (HVP) are crucial inputs to previous and future Standard Model (SM) predictions of the muon’s anomalous magnetic moment, <a:math xmlns:a=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><a:msub><a:mi>a</a:mi><a:mi>μ</a:mi></a:msub></a:math>. With the muon <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mi>g</c:mi><c:mo>−</c:mo><c:mn>2</c:mn></c:math>’s new physics case uncertain due to disagreeing HVP evaluations, new SM predictions and experimental measurements of <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><e:msub><e:mi>a</e:mi><e:mi>μ</e:mi></e:msub></e:math> expected soon, and a complete revamp of the KNTW analysis framework underway, this Letter motivates and describes a blinding scheme for data-driven HVP determinations that has been implemented for future KNTW analyses.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380869854373536257","@type":"Researcher","foaf:name":[{"@value":"Alexander Keshavarzi"}],"jpcoar:affiliationName":[{"@value":"The University of 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(APS)"}],"prism:publicationDate":"2025-01-10","prism:volume":"111","prism:number":"1"},"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.111.L011901"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevD.111.L011901/fulltext"}],"createdAt":"2025-01-10","modifiedAt":"2025-08-05","project":[{"@id":"https://cir.nii.ac.jp/crid/1040285300699479936","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"20K03960"},{"@type":"JGN","@value":"JP20K03960"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-20K03960/"}],"notation":[{"@language":"ja","@value":"ミューオン異常磁気能率を突破口とした新物理探索のための基礎研究"},{"@language":"en","@value":"Basic research for the search for new physics beyond the Standard Model using the muon anomalous magnetic moment as a 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display=\"inline\"><mml:msup><mml:mi>e</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>e</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mo stretchy=\"false\">→</mml:mo><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:mi>γ</mml:mi></mml:math>\n and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>e</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>e</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mo stretchy=\"false\">→</mml:mo><mml:msup><mml:mi>π</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>π</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mi>γ</mml:mi></mml:math>\n at \n<i>BABAR</i>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360869859439660288","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Modeling the R-ratio and hadronic contributions to $$g-2$$ with a Treed Gaussian 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mathvariant=\"normal\">QED</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msubsup><mml:mrow><mml:mo>(</mml:mo><mml:mi>M</mml:mi></mml:mrow><mml:mrow><mml:mi>Z</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msubsup></mml:mrow><mml:mo>)</mml:mo></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137044964794624","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Reevaluation of the hadronic contributions to the muon g−2 and to $\\alpha (M^{2}_{Z})$"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137045335098880","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"$${\\hbox {BHLS}}_2$$, a new breaking of the HLS model and its phenomenology"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137045557851520","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Improved predictions for <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:mi>g</mml:mi><mml:mo>−</mml:mo><mml:mn>2</mml:mn></mml:math> of the muon and <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si2.gif\" overflow=\"scroll\"><mml:msub><mml:mi>α</mml:mi><mml:mi mathvariant=\"normal\">QED</mml:mi></mml:msub><mml:mo stretchy=\"false\">(</mml:mo><mml:msubsup><mml:mi>M</mml:mi><mml:mi>Z</mml:mi><mml:mn>2</mml:mn></mml:msubsup><mml:mo stretchy=\"false\">)</mml:mo></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137046001528576","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Precision measurement of <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:mi>σ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><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:mo>→</mml:mo><mml:msup><mml:mrow><mml:mi>π</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mrow><mml:mi>π</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mi>γ</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mo stretchy=\"false\">/</mml:mo><mml:mi>σ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><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:mo>→</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>μ</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mi>γ</mml:mi><mml:mo stretchy=\"false\">)</mml:mo></mml:math> and determination of the <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si2.gif\" overflow=\"scroll\"><mml:msup><mml:mrow><mml:mi>π</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mrow><mml:mi>π</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:math> contribution to the muon anomaly with the KLOE detector"}]},{"@id":"https://cir.nii.ac.jp/crid/1361412894851991424","@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>g</mml:mi><mml:mo>−</mml:mo><mml:mn>2</mml:mn></mml:math>\n of charged leptons, \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>α</mml:mi><mml:mo mathvariant=\"bold\" stretchy=\"false\">(</mml:mo><mml:msubsup><mml:mi>M</mml:mi><mml:mi>Z</mml:mi><mml:mn>2</mml:mn></mml:msubsup><mml:mo mathvariant=\"bold\" stretchy=\"false\">)</mml:mo></mml:math>\n, and the hyperfine splitting of muonium"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418518555427072","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Dispersion relation for hadronic light-by-light scattering: two-pion 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stretchy=\"false\">)</mml:mo><mml:mi>μ</mml:mi></mml:msub></mml:math>after the Higgs-boson mass measurement"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699994259838720","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Refinements in electroweak contributions to the muon anomalous magnetic moment"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995004400896","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Muon <i>g</i> – 2 theory: The hadronic part"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995247896704","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Leading-order hadronic contribution to the electron and muon<i>g</i>− 2"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699996033277952","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Hadronic light-by-light scattering contribution to the muon anomalous magnetic moment reexamined"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981469967243520","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Leading hadronic contribution to \n<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>\n from lattice QCD with \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>N</mml:mi><mml:mi mathvariant=\"normal\">f</mml:mi></mml:msub><mml:mo>=</mml:mo><mml:mn>2</mml:mn><mml:mo>+</mml:mo><mml:mn>1</mml:mn></mml:math>\n flavors of \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi mathvariant=\"normal\">O</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>a</mml:mi><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:math>\n improved Wilson quarks"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470441871488","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Dispersion relation for hadronic light-by-light scattering: pion pole"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262943799758720","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Measurement of <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:mi>σ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:msup><mml:mi>e</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>e</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mo>→</mml:mo><mml:msup><mml:mi>π</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>π</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mi>γ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>γ</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:mo stretchy=\"false\">)</mml:mo></mml:math> and the dipion contribution to the muon anomaly with the KLOE detector"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262944483080064","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Pseudoscalar-pole contribution to the<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>g</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:msub><mml:mo>−</mml:mo><mml:mn>2</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:math>: A rational approach"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262946416394240","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Longitudinal short-distance constraints for the hadronic light-by-light contribution to (g − 2)μ with large-Nc Regge models"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544419075174528","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Hadronic-vacuum-polarization contribution to the muon’s anomalous magnetic moment from four-flavor lattice QCD"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544419329761152","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Erratum to: Reevaluation of the hadronic contributions to the muon g−2 and to \n                \n                  \n                \n                $\\alpha(M_{Z}^{2})$"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544420259853696","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Higher-order hadronic contributions to the anomalous magnetic moment of leptons"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825894689971200","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Three-pion contribution to hadronic vacuum polarization"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825895139757568","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Measurement of the Positive Muon Anomalous Magnetic Moment to 0.7 ppm"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825895249207936","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"The role of mesons in muon <i>g</i> − 2"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825895508938752","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Measurement of the Negative Muon Anomalous Magnetic Moment to 0.7 ppm"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107368519512192","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Electromagnetic and strong isospin-breaking corrections to the 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 from lattice \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>QCD</mml:mi><mml:mo>+</mml:mo><mml:mtext>QED</mml:mtext></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107368581337472","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Hadronic Vacuum Polarization Contribution to the Anomalous Magnetic Moments of Leptons from First Principles"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107370426662144","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Upgraded breaking of the HLS model: a full solution to the τ−e + e − and ϕ decay issues and its consequences on g−2 VMD estimates"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107370586656000","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Final report of the E821 muon anomalous magnetic moment measurement at BNL"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107370850286592","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"A new evaluation of the hadronic vacuum polarisation contributions to the muon anomalous magnetic moment and to $$\\varvec{\\alpha }({{\\varvec{m}}}_{{\\varvec{Z}}}^2)$$"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107371277936384","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Precise Measurement of the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>e</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>e</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mo>→</mml:mo><mml:msup><mml:mi>π</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>π</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>γ</mml:mi><mml:mo stretchy=\"false\">)</mml:mo></mml:math>Cross Section with the Initial State Radiation Method 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Rev. D<b>67</b>, 073006 (2003)]"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388846275286400","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Remarks on higher-order hadronic corrections to the muon <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:mi>g</mml:mi><mml:mo>−</mml:mo><mml:mn>2</mml:mn></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670320873437952","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Measuring the leading hadronic contribution to the muon g-2 via $$\\mu e$$ μ e scattering"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951794215374464","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"An update of the HLS estimate of the muon g−2"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233268204371968","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Publisher’s Note: Measurement of the Positive Muon Anomalous Magnetic Moment to 0.7 ppm [Phys. Rev. Lett.<b>89</b>, 101804 (2002)]"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233268263232384","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Short-distance constraints for the HLbL contribution to the muon anomalous magnetic moment"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233271198731136","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Hadronic contribution to the muon anomalous magnetic moment to next-to-next-to-leading order"}]},{"@id":"https://cir.nii.ac.jp/crid/2050025942148289536","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"A new approach for measuring the muon anomalous magnetic moment and electric dipole moment"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1103/physrevd.111.l011901"},{"@type":"KAKEN","@value":"PRODUCT-25485226"}]}