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001048507 005__ 20251212202212.0
001048507 0247_ $$2doi$$a10.1016/j.physrep.2025.08.002
001048507 0247_ $$2ISSN$$a0370-1573
001048507 0247_ $$2ISSN$$a1873-6270
001048507 0247_ $$2datacite_doi$$a10.34734/FZJ-2025-04692
001048507 037__ $$aFZJ-2025-04692
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001048507 1001_ $$0P:(DE-HGF)0$$aAliberti, R.$$b0
001048507 245__ $$aThe anomalous magnetic moment of the muon in the Standard Model: an update
001048507 260__ $$aAmsterdam [u.a.]$$bElsevier Science, North-Holland$$c2025
001048507 3367_ $$2DataCite$$aOutput Types/Book Review
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001048507 3367_ $$2ORCID$$aBOOK_REVIEW
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001048507 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$mjournal
001048507 3367_ $$2BibTeX$$aARTICLE
001048507 3367_ $$00$$2EndNote$$aJournal Article
001048507 520__ $$aWe present the current Standard Model (SM) prediction for the muon anomalousmagnetic moment, aμ, updating the first White Paper (WP20) [1]. The pure QED andelectroweak contributions have been further consolidated, while hadronic contributionscontinue to be responsible for the bulk of the uncertainty of the SM prediction. Signifi-cant progress has been achieved in the hadronic light-by-light scattering contributionusing both the data-driven dispersive approach as well as lattice-QCD calculations,leading to a reduction of the uncertainty by almost a factor of two. The most importantdevelopment since WP20 is the change in the estimate of the leading-order hadronic-vacuum-polarization (LO HVP) contribution. A new measurement of the $e^+e^− →π^+π^−$ cross section by CMD-3 has increased the tensions among data-driven dispersiveevaluations of the LO HVP contribution to a level that makes it impossible to combinethe results in a meaningful way. At the same time, the attainable precision of lattice-QCD calculations has increased substantially and allows for a consolidated lattice-QCDaverage of the LO HVP contribution with a precision of about 0.9%. Adopting the latter inthis update has resulted in a major upward shift of the total SM prediction, which nowreads $a^{SM}_μ = 116 592 033(62) × 10^{−11} (530 ppb)$. When compared against the currentexperimental average based on the E821 experiment and runs 1–6 of E989 at Fermilab,one finds $a^{exp}_μ − a^{SM}_μ = 38(63) × 10^{−11}$, which implies that there is no tension betweenthe SM and experiment at the current level of precision. The final precision of E989(127 ppb) is the target of future efforts by the Theory Initiative. The resolution of thetensions among data-driven dispersive evaluations of the LO HVP contribution will be akey element in this endeavor.
001048507 536__ $$0G:(DE-HGF)POF4-5111$$a5111 - Domain-Specific Simulation & Data Life Cycle Labs (SDLs) and Research Groups (POF4-511)$$cPOF4-511$$fPOF IV$$x0
001048507 536__ $$0G:(EU-Grant)101054515$$aMUON - Lattice determination of the muon's anomalous magnetic moment (101054515)$$c101054515$$fERC-2021-ADG$$x1
001048507 588__ $$aDataset connected to CrossRef, Journals: juser.fz-juelich.de
001048507 7001_ $$00009-0009-0491-1024$$aAoyama, T.$$b1
001048507 7001_ $$00009-0005-9971-9473$$aBalzani, E.$$b2
001048507 7001_ $$00000-0003-3183-7316$$aBashir, A.$$b3
001048507 7001_ $$00009-0005-1576-3654$$aBenton, G.$$b4
001048507 7001_ $$00000-0002-1618-2844$$aBijnens, J.$$b5
001048507 7001_ $$00000-0001-5274-9812$$aBiloshytskyi, V.$$b6
001048507 7001_ $$0P:(DE-HGF)0$$aBlum, T.$$b7
001048507 7001_ $$00000-0002-4426-7984$$aBoito, D.$$b8
001048507 7001_ $$00000-0002-5127-4461$$aBruno, M.$$b9
001048507 7001_ $$00009-0001-0999-0878$$aBudassi, E.$$b10
001048507 7001_ $$00000-0002-4487-264X$$aBurri, S.$$b11
001048507 7001_ $$00000-0003-2461-0666$$aCappiello, L.$$b12
001048507 7001_ $$00000-0002-7315-0638$$aCarloni Calame, C. M.$$b13
001048507 7001_ $$00000-0001-6906-6823$$aCè, M.$$b14
001048507 7001_ $$00000-0002-9056-754X$$aCirigliano, V.$$b15
001048507 7001_ $$0P:(DE-HGF)0$$aClarke, D. A.$$b16
001048507 7001_ $$00000-0003-3954-9503$$aColangelo, G.$$b17$$eCorresponding author
001048507 7001_ $$00000-0002-0375-0611$$aCotrozzi, L.$$b18
001048507 7001_ $$00009-0007-3577-4785$$aCottini, M.$$b19
001048507 7001_ $$00000-0001-8950-0770$$aDanilkin, I.$$b20
001048507 7001_ $$00000-0002-0337-1013$$aDavier, M.$$b21$$eCorresponding author
001048507 7001_ $$00000-0003-0047-0689$$aDella Morte, M.$$b22
001048507 7001_ $$00000-0001-7974-5854$$aDenig, A.$$b23
001048507 7001_ $$00000-0002-0216-6771$$aDeTar, C.$$b24
001048507 7001_ $$00000-0003-4983-632X$$aDruzhinin, V.$$b25
001048507 7001_ $$00000-0002-0546-2533$$aEichmann, G.$$b26
001048507 7001_ $$00000-0001-9105-8213$$aEl-Khadra, A. X.$$b27$$eCorresponding author
001048507 7001_ $$0P:(DE-HGF)0$$aEstrada, E.$$b28
001048507 7001_ $$0P:(DE-HGF)0$$aFeng, X.$$b29
001048507 7001_ $$0P:(DE-HGF)0$$aFischer, C. S.$$b30
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001048507 7001_ $$00000-0002-8839-7166$$aGérardin, A.$$b33
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001048507 7001_ $$00000-0001-9471-1740$$aHoid, B.-L.$$b48
001048507 7001_ $$0P:(DE-HGF)0$$aHolz, S.$$b49
001048507 7001_ $$00000-0002-7420-2233$$aHudspith, R. J.$$b50
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001048507 7001_ $$0P:(DE-HGF)0$$aJin, L.$$b52
001048507 7001_ $$00000-0001-6404-545X$$aKalntis, N.$$b53
001048507 7001_ $$00000-0002-4340-4983$$aKanwar, G.$$b54
001048507 7001_ $$00000-0001-9085-7283$$aKeshavarzi, A.$$b55
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001048507 7001_ $$00000-0002-1541-6581$$aKubis, B.$$b59
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001048507 7001_ $$00000-0002-3584-4567$$aLehner, C.$$b64$$eCorresponding author
001048507 7001_ $$00000-0002-2154-9292$$aLellmann, M.$$b65
001048507 7001_ $$00000-0002-0032-6073$$aLellouch, L.$$b66$$eCorresponding author
001048507 7001_ $$00009-0004-5017-0355$$aLeplumey, T.$$b67
001048507 7001_ $$00000-0002-7862-1646$$aLeutgeb, J.$$b68
001048507 7001_ $$0P:(DE-HGF)0$$aLin, T.$$b69
001048507 7001_ $$0P:(DE-HGF)0$$aLiu, Q.$$b70
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001048507 7001_ $$0P:(DE-HGF)0$$aMiller, N.$$b85
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001048507 7001_ $$00000-0002-5279-2316$$aRoberts, B. L.$$b112$$eCorresponding author
001048507 7001_ $$00000-0001-7291-2146$$aRodríguez-Sánchez, A.$$b113
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001048507 7001_ $$00000-0002-9726-8534$$aToelstede, J.-N.$$b126
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001048507 7001_ $$00000-0001-6797-7607$$aTorres Bobadilla, W. J.$$b128
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