HackerPapers

arXiv:2505.21476hep-ph

The anomalous magnetic moment of the muon in the Standard Model: an update

R. Aliberti, T. Aoyama, E. Balzani, A. Bashir, G. Benton, J. Bijnens, V. Biloshytskyi, T. Blum, D. Boito, M. Bruno, E. Budassi, S. Burri, L. Cappiello, C. M. Carloni Calame, M. Cè, V. Cirigliano, D. A. Clarke, G. Colangelo, L. Cotrozzi, M. Cottini, I. Danilkin, M. Davier, M. Della Morte, A. Denig, C. DeTar, V. Druzhinin, G. Eichmann, A. X. El-Khadra, E. Estrada, X. Feng, C. S. Fischer, R. Frezzotti, G. Gagliardi, A. Gérardin, M. Ghilardi, D. Giusti, M. Golterman, S. Gonzàlez-Solís, S. Gottlieb, R. Gruber, A. Guevara, V. Gülpers, A. Gurgone, F. Hagelstein, M. Hayakawa, N. Hermansson-Truedsson, A. Hoecker, M. Hoferichter, B. -L. Hoid, S. Holz, R. J. Hudspith, F. Ignatov, L. Jin, N. Kalntis, G. Kanwar, A. Keshavarzi, J. Komijani, J. Koponen, S. Kuberski, B. Kubis, A. Kupich, A. Kupść, S. Lahert, S. Laporta, C. Lehner, M. Lellmann, L. Lellouch, T. Leplumey, J. Leutgeb, T. Lin, Q. Liu, I. Logashenko, C. Y. London, G. López Castro, J. Lüdtke, A. Lusiani, A. Lutz, J. Mager, B. Malaescu, K. Maltman, M. K. Marinković, J. Márquez, P. Masjuan, H. B. Meyer, T. Mibe, N. Miller, A. Miramontes, A. Miranda, G. Montagna, S. E. Müller, E. T. Neil, A. V. Nesterenko, O. Nicrosini, M. Nio, D. Nomura, J. Paltrinieri, L. Parato, J. Parrino, V. Pascalutsa, M. Passera, S. Peris, P. Petit Rosàs, F. Piccinini, R. N. Pilato, L. Polat, A. Portelli, D. Portillo-Sánchez, M. Procura, L. Punzi, K. Raya, A. Rebhan, C. F. Redmer, B. L. Roberts, A. Rodríguez-Sánchez, P. Roig, J. Ruiz de Elvira, P. Sánchez-Puertas, A. Signer, J. W. Sitison, D. Stamen, D. Stöckinger, H. Stöckinger-Kim, P. Stoffer, Y. Sue, P. Tavella, T. Teubner, J. -N. Toelstede, G. Toledo, W. J. Torres Bobadilla, J. T. Tsang, F. P. Ucci, Y. Ulrich, R. S. Van de Water, G. Venanzoni, S. Volkov, G. von Hippel, G. Wang, U. Wenger, H. Wittig, A. Wright, E. Zaid, M. Zanke, Z. Zhang, M. Zillinger, C. Alexandrou, A. Altherr, M. Anderson, C. Aubin, S. Bacchio, P. Beltrame, A. Beltran, P. Boyle, I. Campos Plasencia, I. Caprini, B. Chakraborty, G. Chanturia, A. Crivellin, A. Czarnecki, L. -Y. Dai, T. Dave, L. Del Debbio, K. Demory, D. Djukanovic, T. Draper, A. Driutti, M. Endo, F. Erben, K. Ferraby, J. Finkenrath, L. Flower, A. Francis, E. Gámiz, J. Gogniat, A. V. Grebe, S. Gündogdu, M. T. Hansen, S. Hashimoto, H. Hayashii, D. W. Hertzog, L. A. Heuser, L. Hostetler, X. T. Hou, G. S. Huang, T. Iijima, K. Inami, A. Jüttner, R. Kitano, M. Knecht, S. Kollatzsch, A. S. Kronfeld, T. Lenz, G. Levati, Q. M. Li, Y. P. Liao, J. Libby, K. F. Liu, V. Lubicz, M. T. Lynch, A. T. Lytle, J. L. Ma, K. Miura, K. Möhling, J. Muskalla, F. Noël, K. Ottnad, P. Paradisi, C. T. Peterson, A. Pich, S. Pitelis, S. Plura, A. Price, D. Radic, A. Radzhabov, A. Risch, S. Romiti, S. Sahoo, F. Sannino, H. Schäfer, Y. Schelhaas, S. I. Serednyakov, O. Shekhovtsova, J. N. Simone, S. Simula, E. P. Solodov, F. M. Stokes, M. Vanderhaeghen, A. Vaquero, N. Vestergaard, W. P. Wang, Z. Wąs, K. Yamashita, Y. B. Yang, T. Yoshioka, C. Z. Yuan, A. S. Zhevlakov

HN submission. Found in a submission link or body. Submitters do not count as commenters in the main ranking; a submission is not an endorsement.

Abstract

We present the current Standard Model (SM) prediction for the muon anomalous magnetic moment, $a_μ$, updating the first White Paper (WP20) [1]. The pure QED and electroweak contributions have been further consolidated, while hadronic contributions continue to be responsible for the bulk of the uncertainty of the SM prediction. Significant progress has been achieved in the hadronic light-by-light scattering contribution using 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 important development since WP20 is the change in the estimate of the leading-order hadronic-vacuum-polarization (LO HVP) contribution. A new measurement of the $e^+e^-\toπ^+π^-$ cross section by CMD-3 has increased the tensions among data-driven dispersive evaluations of the LO HVP contribution to a level that makes it impossible to combine the 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-QCD average of the LO HVP contribution with a precision of about 0.9%. Adopting the latter in this update has resulted in a major upward shift of the total SM prediction, which now reads $a_μ^\text{SM} = 116\,592\,033(62)\times 10^{-11}$ (530 ppb). When compared against the current experimental average based on the E821 experiment and runs 1-6 of E989 at Fermilab, one finds $a_μ^\text{exp} - a_μ^\text{SM} =38(63)\times 10^{-11}$, which implies that there is no tension between the 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 the tensions among data-driven dispersive evaluations of the LO HVP contribution will be a key element in this endeavor.

arXiv comments
188 pages, 83 figures; $a_μ^\text{exp}$ updated to final result of the Fermilab experiment, SM prediction unchanged; journal version
Journal reference
Phys. Rept. 1143 (2025) 1-158
DOI
doi:10.1016/j.physrep.2025.08.002
Subjects
hep-phHigh Energy Physics, Phenomenology hep-exHigh Energy Physics, Experiment hep-latHigh Energy Physics, Lattice nucl-exNuclear Experiment nucl-thNuclear Theory

On Hacker News

No comments linking this paper were found in the collected sources. Found in 1 HN submission from May 2025 to May 2025. Open submission discussions.

Comments linking this paper, per year.

Discussed in comments0 threads

No comments linking this paper were found in the collected sources. Open submission discussions.

Submitted to Hacker News

Connected through shared HN threads, not inferred similarity or a recommendation.