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Hadronic corrections to the muon lifetime are calculated in the Fermi theory in the presence of QED using dispersion relations. The result, after convolution of hadron data with the calculated perturbative kernel is Delta Gamma_had =…

High Energy Physics - Phenomenology · Physics 2009-10-31 Timo van Ritbergen , Robin G. Stuart

A fundamental property of QCD is the presence of the chiral anomaly, which is the primary component of the $\pi^0\rightarrow\gamma\gamma$ decay amplitude. Based on this anomaly and its small ($\simeq$ 4.5%) chiral correction, a firm…

High Energy Physics - Phenomenology · Physics 2015-06-03 A. M. Bernstein , Barry R. Holstein

The Muon g-2 experiment at Fermilab will measure the anomalous magnetic moment of the muon to a precision of 140 parts per billion, which is a factor of four improvement over the previous E821 measurement at Brookhaven. The experiment will…

High Energy Physics - Experiment · Physics 2018-07-01 J. L. Holzbauer

We propose to measure the rate \Rd\ for muon capture on the deuteron to better than 1.5% precision. This process is the simplest weak interaction process on a nucleus that can both be calculated and measured to a high degree of precision.…

The tau lepton lifetime is measured with the L3 detector at LEP using the complete data taken at centre-of-mass energies around the Z pole resulting in tau_tau = 293.2 +/- 2.0 (stat) +/- 1.5 (syst) fs. The comparison of this result with the…

High Energy Physics - Experiment · Physics 2012-08-27 L3 Collaboration

Experimental measurement of the probability of direct decay of a pion into a positron allows searching for interactions beyond the Standard Model: test of the hypothesis about the universality of the charged current,search for new…

Instrumentation and Detectors · Physics 2020-10-05 Vladimir I. Selivanov

Muons can serve as probes to precisely determine fundamental parameters of the Standard Model or search for `new physics'. The high intensity muon beams at the Paul Scherrer Institut (PSI) allow for precision measurements and searches for…

Nuclear Experiment · Physics 2010-02-25 Bernhard Lauss

This article reviews the muon g-2 experiment, a cornerstone in precision tests of the Standard Model of particle physics. The experiment measures the anomalous magnetic moment of the muon with unprecedented accuracy, seeking potential…

High Energy Physics - Experiment · Physics 2025-08-06 Marin Karuza

The Quasiparticle Random Phase Approximation (QRPA) is used in evaluation of the total muon capture ratesfor the final nuclei participating in double-beta decay. Several variants of the method are used, depending on the size of the single…

Nuclear Theory · Physics 2020-09-09 Fedor Simkovic , Rastislav Dvornicky , Petr Vogel

We have measured the optically injected excess carrier lifetime in silicon using photoexcited muon spin spectroscopy. Positive muons implanted deep in a wafer can interact with the excess carriers and directly probe the bulk carrier…

Materials Science · Physics 2017-12-06 K. Yokoyama , J. S. Lord , J. Miao , P. Murahari , A. J. Drew

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

Muons, as a bulk probe of materials, have been used to study the depth profile of charge carrier kinetics in Si wafers by scanning the muon implantation depth. The photoexcited muon spin spectroscopy technique can optically generate excess…

Materials Science · Physics 2021-07-07 K. Yokoyama , J. S. Lord , J. Miao , P. Murahari , A. J. Drew

In a typical experiment the nuclear \mu-capture rate is determined from measurements of the time constant of the muon decay exponential in a target. We propose a new approach for the evaluation of the \mu-capture rate, which is based on…

Nuclear Experiment · Physics 2013-03-05 S. N. Gninenko

A new experiment at Fermilab will measure the anomalous magnetic moment of the muon with a precision of 140 parts per billion (ppb). This measurement is motivated by the results of the Brookhaven E821 experiment that were first released…

Instrumentation and Detectors · Physics 2015-10-02 Frederick Gray

We describe a compact apparatus that automatically measures the charge averaged lifetime of atmospheric muons in plastic scintillator using low-cost, low-power electronics and that measures the stopping rate of atmospheric muons as a…

Instrumentation and Detectors · Physics 2015-06-26 Thomas Coan , Tiankuan Liu , Jingbo Ye

The new g-2 experiment at Fermilab aims to measure the muon anomalous magnetic moment by a fourfold improvement in precision compared to the BNL experiment. Achieving this goal requires the delivery of highly polarized 3.094 GeV/c muons…

The Muon g-2 Experiment at Fermilab will measure the anomalous magnetic moment of the muon to a precision of 140 parts per billion, which is a factor of four improvement over the previous E821 measurement at Brookhaven. The experiment will…

Instrumentation and Detectors · Physics 2017-01-04 J. L. Holzbauer

The muon capture rate in the reaction mu- 3He -> nu + 3H has been measured at PSI using a modular high pressure ionization chamber. The rate corresponding to statistical hyperfine population of the mu-3He atom is (1496.0 +- 4.0) s^-1. This…

An instructional laboratory experiment to measure the muon mass is described. Using coincidence-anticoincidence detection, the decay of a cosmic-ray muon into an electron (or positron) is observed in a multiplate spark chamber, and recorded…

Physics Education · Physics 2010-02-05 Benjamin Brau , Christopher May , Robert Ormond , John Essick