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The muon g-2 experiment at Brookhaven National Laboratory measures the anomalous magnetic moment of the muon, $a_\mu$, very precisely. This measurement tests the Standard Model. The analysis for the data collected in 2000 (a $\mu^+$ run) is…

High Energy Physics - Experiment · Physics 2019-08-14 Cenap S. Ozben

The E989 Muon $g-2$ experiment at Fermilab aims to measure the anomalous magnetic moment, $a^{}_\mu$, of the muon with a precision of 140 parts-per-billion. This requires a precise measurement of both the anomalous spin precession…

Instrumentation and Detectors · Physics 2021-02-11 S. Corrodi , P. De Lurgio , D. Flay , J. Grange , R. Hong , D. Kawall , M. Oberling , S. Ramachandran , P. Winter

The Mu2e experiment at Fermilab is being designed to study the coherent neutrino-less conversion of a negative muon into an electron in the field of a nucleus. This process has an extremely low probability in the Standard Model and its…

Accelerator Physics · Physics 2017-10-11 V. Pronskikh , D. Glenzinski , N. Mokhov , R. Tschirhart

The new CDF II measurement of $W$-boson mass shows a 7$\sigma$ deviation from the Standard Model (SM) prediction, while the recent FNAL measurement of the muon $g-2$ shows a 4.2$\sigma$ deviation (combined with the BNL result) from the SM.…

High Energy Physics - Phenomenology · Physics 2022-06-14 Jin Min Yang , Yang Zhang

The Fermi National Accelerator Laboratory (FNAL) Muon $g-2$ Experiment has measured the positive muon magnetic anomaly $a_{\mu} \equiv (g_{\mu}-2)/2$ with a precision of 0.46 parts per million, with data collected during its first physics…

High Energy Physics - Experiment · Physics 2022-03-07 Alessandra Lucà

A new measurement of the magnetic anomaly $a_{\mu}$ of the positive muon is presented based on data taken from 2020 to 2023 by the Muon $g-2$ Experiment at Fermi National Accelerator Laboratory (FNAL). This dataset contains over 2.5 times…

High Energy Physics - Experiment · Physics 2025-06-04 The Muon $g-2$ Collaboration , : , D. P. Aguillard , T. Albahri , D. Allspach , J. Annala , K. Badgley , S. Baeßler , I. Bailey , L. Bailey , E. Barlas-Yucel , T. Barrett , E. Barzi , F. Bedeschi , M. Berz , M. Bhattacharya , H. P. Binney , P. Bloom , J. Bono , E. Bottalico , T. Bowcock , S. Braun , M. Bressler , G. Cantatore , R. M. Carey , B. C. K. Casey , D. Cauz , R. Chakraborty , A. Chapelain , S. Chappa , S. Charity , C. Chen , M. Cheng , R. Chislett , Z. Chu , T. E. Chupp , C. Claessens , F. Confortini , M. E. Convery , S. Corrodi , L. Cotrozzi , J. D. Crnkovic , S. Dabagov , P. T. Debevec , S. Di Falco , G. Di Sciascio , S. Donati , B. Drendel , A. Driutti , M. Eads , A. Edmonds , J. Esquivel , M. Farooq , R. Fatemi , K. Ferraby , C. Ferrari , M. Fertl , A. T. Fienberg , A. Fioretti , D. Flay , S. B. Foster , H. Friedsam , N. S. Froemming , C. Gabbanini , I. Gaines , S. Ganguly , J. George , L. K. Gibbons , A. Gioiosa , K. L. Giovanetti , P. Girotti , W. Gohn , L. Goodenough , T. Gorringe , J. Grange , S. Grant , F. Gray , S. Haciomeroglu , T. Halewood-Leagas , D. Hampai , F. Han , J. Hempstead , D. W. Hertzog , G. Hesketh , E. Hess , A. Hibbert , Z. Hodge , S. Y. Hoh , K. W. Hong , R. Hong , T. Hu , Y. Hu , M. Iacovacci , M. Incagli , S. Israel , P. Kammel , M. Kargiantoulakis , M. Karuza , J. Kaspar , D. Kawall , L. Kelton , A. Keshavarzi , D. S. Kessler , K. S. Khaw , Z. Khechadoorian , B. Kiburg , M. Kiburg , O. Kim , N. Kinnaird , E. Kraegeloh , J. LaBounty , K. R. Labe , M. Lancaster , S. Lee , B. Li , D. Li , L. Li , I. Logashenko , A. Lorente Campos , Z. Lu , A. Lucà , G. Lukicov , A. Lusiani , A. L. Lyon , B. MacCoy , R. Madrak , K. Makino , S. Mastroianni , R. McCarthy , J. P. Miller , S. Miozzi , B. Mitra , J. P. Morgan , W. M. Morse , J. Mott , A. Nath , J. K. Ng , H. Nguyen , Y. Oksuzian , Z. Omarov , W. Osar , R. Osofsky , S. Park , G. Pauletta , J. Peck , G. M. Piacentino , R. N. Pilato , K. T. Pitts , B. Plaster , N. Pohlman , C. C. Polly , D. Počanić , J. Price , B. Quinn , M. U. H. Qureshi , G. Rakness , S. Ramachandran , E. Ramberg , R. Reimann , B. L. Roberts , D. L. Rubin , M. Sakurai , L. Santi , C. Schlesier , A. Schreckenberger , Y. K. Semertzidis , M. Sorbara , J. Stapleton , D. Still , C. Stoughton , D. Stratakis , D. Stöckinger , H. E. Swanson , G. Sweetmore , D. A. Sweigart , M. J. Syphers , Y. Takeuchi , D. A. Tarazona , T. Teubner , A. E. Tewsley-Booth , V. Tishchenko , N. H. Tran , W. Turner , E. Valetov , D. Vasilkova , G. Venanzoni , T. Walton , A. Weisskopf , L. Welty-Rieger , P. Winter , Y. Wu , B. Yu , M. Yucel , E. Zaid , Y. Zeng , C. Zhang

This paper introduces a new approach to measure the muon magnetic moment anomaly $a_{\mu} = (g-2)/2$, and the muon electric dipole moment (EDM) $d_{\mu}$ at the J-PARC muon facility. The goal of our experiment is to measure $a_{\mu}$ and…

The latest results of anomalous muon magnetic moment at Fermilab show a discrepancy of 4.2 $\sigma$ between the Standard Model (SM) prediction and experimental value. In this work, we revisit $U(1)_{L_{\mu}-L_{\tau}}$ symmetry with in the…

High Energy Physics - Phenomenology · Physics 2023-02-08 Simran Arora , Monal Kashav , Surender Verma , B. C. Chauhan

We consider a type I or type X two Higgs doublets model with a modified lepton sector. The generalized lepton sector is also flavor conserving but with the new Yukawa couplings completely decoupled from lepton mass proportionality. The…

High Energy Physics - Phenomenology · Physics 2023-02-08 Francisco J. Botella , Fernando Cornet-Gomez , Carlos Miró , Miguel Nebot

Current experimental data from the $g-2$ muon factor, seems to show the necessity of physics beyond the Standard Model (SM), since the difference between SM and experimental predictions is 2.6$\sigma $. In the framework of the General Two…

High Energy Physics - Phenomenology · Physics 2013-05-29 Rodolfo A. Diaz , R. Martinez , J. -Alexis Rodriguez

We present details on a new measurement of the muon magnetic anomaly, $a_\mu = (g_\mu -2)/2$. The result is based on positive muon data taken at Fermilab's Muon Campus during the 2019 and 2020 accelerator runs. The measurement uses $3.1$…

High Energy Physics - Experiment · Physics 2024-05-24 D. P. Aguillard , T. Albahri , D. Allspach , A. Anisenkov , K. Badgley , S. Baeßler , I. Bailey , L. Bailey , V. A. Baranov , E. Barlas-Yucel , T. Barrett , E. Barzi , F. Bedeschi , M. Berz , M. Bhattacharya , H. P. Binney , P. Bloom , J. Bono , E. Bottalico , T. Bowcock , S. Braun , M. Bressler , G. Cantatore , R. M. Carey , B. C. K. Casey , D. Cauz , R. Chakraborty , A. Chapelain , S. Chappa , S. Charity , C. Chen , M. Cheng , R. Chislett , Z. Chu , T. E. Chupp , C. Claessens , M. E. Convery , S. Corrodi , L. Cotrozzi , J. D. Crnkovic , S. Dabagov , P. T. Debevec , S. Di Falco , G. Di Sciascio , S. Donati , B. Drendel , A. Driutti , V. N. Duginov , M. Eads , A. Edmonds , J. Esquivel , M. Farooq , R. Fatemi , C. Ferrari , M. Fertl , A. T. Fienberg , A. Fioretti , D. Flay , S. B. Foster , H. Friedsam , N. S. Froemming , C. Gabbanini , I. Gaines , M. D. Galati , S. Ganguly , A. Garcia , J. George , L. K. Gibbons , A. Gioiosa , K. L. Giovanetti , P. Girotti , W. Gohn , L. Goodenough , T. Gorringe , J. Grange , S. Grant , F. Gray , S. Haciomeroglu , T. Halewood-Leagas , D. Hampai , F. Han , J. Hempstead , D. W. Hertzog , G. Hesketh , E. Hess , A. Hibbert , Z. Hodge , K. W. Hong , R. Hong , T. Hu , Y. Hu , M. Iacovacci , M. Incagli , P. Kammel , M. Kargiantoulakis , M. Karuza , J. Kaspar , D. Kawall , L. Kelton , A. Keshavarzi , D. S. Kessler , K. S. Khaw , Z. Khechadoorian , N. V. Khomutov , B. Kiburg , M. Kiburg , O. Kim , N. Kinnaird , E. Kraegeloh , V. A. Krylov , N. A. Kuchinskiy , K. R. Labe , J. LaBounty , M. Lancaster , S. Lee , B. Li , D. Li , L. Li , I. Logashenko , A. Lorente Campos , Z. Lu , A. Lucà , G. Lukicov , A. Lusiani , A. L. Lyon , B. MacCoy , R. Madrak , K. Makino , S. Mastroianni , J. P. Miller , S. Miozzi , B. Mitra , J. P. Morgan , W. M. Morse , J. Mott , A. Nath , J. K. Ng , H. Nguyen , Y. Oksuzian , Z. Omarov , R. Osofsky , S. Park , G. Pauletta , G. M. Piacentino , R. N. Pilato , K. T. Pitts , B. Plaster , D. Počanić , N. Pohlman , C. C. Polly , J. Price , B. Quinn , M. U. H. Qureshi , S. Ramachandran , E. Ramberg , R. Reimann , B. L. Roberts , D. L. Rubin , M. Sakurai , L. Santi , C. Schlesier , A. Schreckenberger , Y. K. Semertzidis , D. Shemyakin , M. Sorbara , J. Stapleton , D. Still , D. Stöckinger , C. Stoughton , D. Stratakis , H. E. Swanson , G. Sweetmore , D. A. Sweigart , M. J. Syphers , D. A. Tarazona , T. Teubner , A. E. Tewsley-Booth , V. Tishchenko , N. H. Tran , W. Turner , E. Valetov , D. Vasilkova , G. Venanzoni , V. P. Volnykh , T. Walton , A. Weisskopf , L. Welty-Rieger , P. Winter , Y. Wu , B. Yu , M. Yucel , Y. Zeng , C. Zhang

Within the Standard Model, in spite of neutrino oscillations, the flavor of charged leptons is conserved in very good approximation, and therefore charged Lepton Flavor Violation is expected to be unobservable. On the other hand, most new…

High Energy Physics - Experiment · Physics 2014-10-20 Francesco Renga

The electron and muon anomalous magnetic moments (AMM) are measured in experiments and studied in the Standard Model (SM) with the highest precision accessible in particle physics. The comparison of the measured quantity with the SM…

High Energy Physics - Phenomenology · Physics 2015-06-19 A. E. Dorokhov , A. E. Radzhabov , A. S. Zhevlakov

We show an interesting correlation between the recent high precision measurement of the $W$-boson mass by the CDF collaboration and the muon $(g-2)$ anomaly in the context of the two Higgs doublet model. One-loop diagrams involving the…

High Energy Physics - Phenomenology · Physics 2022-09-16 K. S. Babu , Sudip Jana , Vishnu P. K.

We propose a simple unified description of two recent precision measurements which suggest new physics beyond the Standard Model of particle interactions, i.e. the deviation of $\sin^2 \theta_W$ in deep inelastic neutrino-nucleon scattering…

High Energy Physics - Phenomenology · Physics 2009-11-07 Ernest Ma , D. P. Roy

The long-standing discrepancy between the experimental determination by the Muon $g-2$ Collaboration at Brookhaven and the Standard Model predictions for the anomalous magnetic moment of the muon cannot be explained within simple unified…

High Energy Physics - Phenomenology · Physics 2017-11-08 Arghya Choudhury , Soumya Rao , Leszek Roszkowski

We review how the muon anomalous magnetic moment ($g-2$) and the quest for lepton flavor violation are intimately correlated. Indeed the decay $\mu \to e \gamma$ is induced by the same amplitude for different choices of in- and outgoing…

High Energy Physics - Phenomenology · Physics 2017-12-08 Manfred Lindner , Moritz Platscher , Farinaldo S. Queiroz

QED, Hadronic, and Electroweak Standard Model contributions to the muon anomalous magnetic moment, a_mu = (g_mu-2)/2, and their theoretical uncertainties are scrutinized. The status and implications of the recently reported 2.6 sigma…

High Energy Physics - Phenomenology · Physics 2009-11-07 Andrzej Czarnecki , William J. Marciano

The current experimental values of anomalous magnetic moments of muon and electron deviate from the Standard Model predictions by few standard deviations, which might be a hint of new physics. The sizes and signs of these deviations are…

High Energy Physics - Phenomenology · Physics 2019-10-23 Marcin Badziak , Kazuki Sakurai

While the muon $g-2$ anomaly can be successfully explained by some new physics models, most of them are severely constrained by the $\mu \to e \gamma$ bound. This tension is more transparent from the effective field theory perspective, in…

High Energy Physics - Phenomenology · Physics 2015-01-20 Wei-Chi Chiu , Chao-Qiang Geng , Da Huang