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Related papers: Workshop on a future muon program at FNAL

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The Mu2e experiment measures the conversion rate of muons into electrons and the Muon g-2 experiment measures the muon magnetic moment. Both experiments require 53 MHz batches of 8 GeV protons to be re-bunched into 150 ns, 2.5 MHz pulses…

Accelerator Physics · Physics 2018-03-28 P. Varghese , B. Chase

The status of the research on muon colliders is discussed and plans are outlined for future theoretical and experimental studies. Besides continued work on the parameters of a 3-4 and 0.5 TeV center-of-mass (CoM) energy collider, many…

Accelerator Physics · Physics 2009-04-17 Charles M. Ankenbrandt

Muon colliders and neutrino factories are attractive options for future facilities aimed at achieving the highest lepton-antilepton collision energies and precision measurements of Higgs boson and neutrino mixing matrix parameters. The…

Accelerator Physics · Physics 2019-08-14 Daniel M. Kaplan

The eventual prospect of muon colliders reaching several TeV encourages us to consider the experimental opportunities presented by very copious stores of muons, approaching $10^{21}$ per year. I summarize and comment upon some highlights of…

High Energy Physics - Phenomenology · Physics 2009-10-31 Chris Quigg

A new measurement of the anomalous magnetic moment of the muon, $a_{\mu} \equiv (g-2)/2$, will be performed at the Fermi National Accelerator Laboratory with data taking beginning in 2017. The most recent measurement, performed at…

High Energy Physics - Experiment · Physics 2018-01-03 Wesley Gohn

The Muon g-2/EDM Experiment at J-PARC will employ a novel way to measure the muon magnetic anomaly, a_mu = (g-2)_mu/2, by using a low-emittance beam of positive muons stored in a compact muon storage magnet. The experimental method includes…

High Energy Physics - Experiment · Physics 2025-12-24 Graziano Venanzoni

The Muon g-2 Experiment at Fermi National Accelerator Laboratory (FNAL) has measured the muon anomalous precession frequency $\omega_a$ to an uncertainty of 434 parts per billion (ppb), statistical, and 56 ppb, systematic, with data…

High Energy Physics - Experiment · Physics 2021-04-08 T. Albahri , A. Anastasi , A. Anisenkov , K. Badgley , S. Baeßler , I. Bailey , V. A. Baranov , E. Barlas-Yucel , T. Barrett , A. Basti , F. Bedeschi , M. Berz , M. Bhattacharya , H. P. Binney , P. Bloom , J. Bono , E. Bottalico , T. Bowcock , G. Cantatore , R. M. Carey , B. C. K. Casey , D. Cauz , R. Chakraborty , S. P. Chang , A. Chapelain , S. Charity , R. Chislett , J. Choi , Z. Chu , T. E. Chupp , S. Corrodi , L. Cotrozzi , J. D. Crnkovic , S. Dabagov , P. T. Debevec , S. Di Falco , P. Di Meo , G. Di Sciascio , R. Di Stefano , A. Driutti , V. N. Duginov , M. Eads , J. Esquivel , M. Farooq , R. Fatemi , C. Ferrari , M. Fertl , A. T. Fienberg , A. Fioretti , D. Flay , E. Frlež , N. S. Froemming , J. Fry , C. Gabbanini , M. D. Galati , S. Ganguly , A. Garcia , J. George , L. K. Gibbons , A. Gioiosa , K. L. Giovanetti , P. Girotti , W. Gohn , T. Gorringe , J. Grange , S. Grant , F. Gray , S. Haciomeroglu , T. Halewood-Leagas , D. Hampai , F. Han , J. Hempstead , A. T. Herrod , D. W. Hertzog , G. Hesketh , A. Hibbert , Z. Hodge , J. L. Holzbauer , K. W. Hong , R. Hong , M. Iacovacci , M. Incagli , P. Kammel , M. Kargiantoulakis , M. Karuza , J. Kaspar , D. Kawall , L. Kelton , A. Keshavarzi , D. Kessler , K. S. Khaw , Z. Khechadoorian , N. V. Khomutov , B. Kiburg , M. Kiburg , O. Kim , Y. I. Kim , B. King , N. Kinnaird , E. Kraegeloh , A. Kuchibhotla , N. A. Kuchinskiy , K. R. Labe , J. LaBounty , M. Lancaster , M. J. Lee , S. Lee , S. Leo , B. Li , D. Li , L. Li , I. Logashenko , A. Lorente Campos , A. Lucà , G. Lukicov , A. Lusiani , A. L. Lyon , B. MacCoy , R. Madrak , K. Makino , F. Marignetti , S. Mastroianni , J. P. Miller , S. Miozzi , W. M. Morse , J. Mott , A. Nath , H. Nguyen , 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 , N. Raha , S. Ramachandran , E. Ramberg , J. L. Ritchie , B. L. Roberts , D. L. Rubin , L. Santi , C. Schlesier , A. Schreckenberger , Y. K. Semertzidis , D. Shemyakin , M. W. Smith , M. Sorbara , D. Stöckinger , J. Stapleton , C. Stoughton , D. Stratakis , T. Stuttard , H. E. Swanson , G. Sweetmore , D. A. Sweigart , M. J. Syphers , D. A. Tarazona , T. Teubner , A. E. Tewsley-Booth , K. Thomson , V. Tishchenko , N. H. Tran , W. Turner , E. Valetov , D. Vasilkova , G. Venanzoni , T. Walton , A. Weisskopf , L. Welty-Rieger , P. Winter , A. Wolski , W. Wu

The goal of the FNAL E989 experiment is to measure the muon magnetic anomaly to unprecedented accuracy and precision at the Fermi National Accelerator Laboratory. To meet this goal, the time and space averaged magnetic environment in the…

We propose an evolution of the Mu2e experiment, called Mu2e-II, that would leverage advances in detector technology and utilize the increased proton intensity provided by the Fermilab PIP-II upgrade to improve the sensitivity for…

Instrumentation and Detectors · Physics 2018-02-09 F. Abusalma , D. Ambrose , A. Artikov , R. Bernstein , G. C. Blazey , C. Bloise , S. Boi , T. Bolton , J. Bono , R. Bonventre , D. Bowring , D. Brown , D. Brown , K. Byrum , M. Campbell , J. -F. Caron , F. Cervelli , D. Chokheli , K. Ciampa , R. Ciolini , R. Coleman , D. Cronin-Hennessy , R. Culbertson , M. A. Cummings , A. Daniel , Y. Davydov , S. Demers , D. Denisov , S. Denisov , S. Di Falco , E. Diociaiuti , R. Djilkibaev , S. Donati , R. Donghia , G. Drake , E. C. Dukes , B. Echenard , A. Edmonds , R. Ehrlich , V. Evdokimov , P. Fabbricatore , A. Ferrari , M. Frank , A. Gaponenko , C. Gatto , Z. Giorgio , S. Giovannella , V. Giusti , H. Glass , D. Glenzinski , L. Goodenough , C. Group , F. Happacher , L. Harkness-Brennan , D. Hedin , K. Heller , D. Hitlin , A. Hocker , R. Hooper , G. Horton-Smith , C. Hu , P. Q. Hung , E. Hungerford , M. Jenkins , M. Jones , M. Kargiantoulakis , K. S. Khaw , B. Kiburg , Y. Kolomensky , J. Kozminski , R. Kutschke , M. Lancaster , D. Lin , I. Logashenko , V. Lombardo , A. Luca , G. Lukicov , K. Lynch , M. Martini , A. Mazzacane , J. Miller , S. Miscetti , L. Morescalchi , J. Mott , S. E. Mueller , P. Murat , V. Nagaslaev , D. Neuffer , Y. Oksuzian , D. Pasciuto , E. Pedreschi , G. Pezzullo , A. Pla-Dalmau , B. Pollack , A. Popov , J. Popp , F. Porter , E. Prebys , V. Pronskikh , D. Pushka , J. Quirk , G. Rakness , R. Ray , M. Ricci , M. Röhrken , V. Rusu , A. Saputi , I. Sarra , M. Schmitt , F. Spinella , D. Stratakis , T. Strauss , R. Talaga , V. Tereshchenko , N. Tran , R. Tschirhart , Z. Usubov , M. Velasco , R. Wagner , Y. Wang , S. Werkema , J. Whitmore , P. Winter , L. Xia , L. Zhang , R. -Y. Zhu , V. Zutshi , R. Zwaska

Muon colliders and neutrino factories are attractive options for future facilities aimed at achieving the highest lepton-antilepton collision energies and precision measurements of parameters of the Higgs boson and the neutrino mixing…

Accelerator Physics · Physics 2019-08-14 Daniel M. Kaplan

With the planned turn-on of the PIP-II 800 MeV superconducting proton linac, Fermilab will potentially become the world's best laboratory at which to carry out fundamental muon measurements, sensitive searches for symmetry violation, and…

An observation of Charged Lepton Flavor Violation (CLFV) would be unambiguous evidence for physics beyond the Standard Model. The Mu2e and COMET experiments, under construction, are designed to push the sensitivity to CLFV in the mu to e…

High Energy Physics - Experiment · Physics 2022-03-17 K. Byrum , S. Corrodi , Y. Oksuzian , P. Winter , L. Xia , A. W. J. Edmonds , J. P. Miller , J. Mott , W. J. Marciano , R. Szafron , R. Bonventre , D. N. Brown , Yu. G. Kolomensky , O. Ning , V. Singh , E. Prebys , L. Borrel , B. Echenard , D. G. Hitlin , C. Hu , D. X. Lin , S. Middleton , F. C. Porter , L. Zhang , R. -Y. Zhu , D. Ambrose , K. Badgley , R. H. Bernstein , S. Boi , B. C. K. Casey , R. Culbertson , A. Gaponenko , H. D. Glass , D. Glenzinski , L. Goodenough , A. Hocker , M. Kargiantoulakis , V. Kashikhin , B. Kiburg , R. K. Kutschke , P. A. Murat , D. Neuffer , V. S. Pronskikh , D. Pushka , G. Rakness , T. Strauss , M. Yucel , C. Bloise , E. Diociaiuti , S. Giovannella , F. Happacher , S. Miscetti , I. Sarra , M. Martini , A. Ferrari , S. E. Müller , R. Rachamin , E. Barlas-Yucel , A. Artikov , N. Atanov , Yu. I. Davydov , V. Glagolev , I. I. Vasilyev , D. N. Brown , Y. Uesaka , S. P. Denisov , V. Evdokimov , A. V. Kozelov , A. V. Popov , I. A. Vasilyev , G. Tassielli , T. Teubner , R. T. Chislett , G. G. Hesketh , M. Lancaster , M. Campbell , K. Ciampa , K. Heller , B. Messerly , M. A. C. Cummings , L. Calibbi , G. C. Blazey , M. J. Syphers , V. Zutshi , C. Kampa , M. MacKenzie , S. Di Falco , S. Donati , A. Gioiosa , V. Giusti , L. Morescalchi , D. Pasciuto , E. Pedreschi , F. Spinella , M. T. Hedges , M. Jones , Z. Y. You , A. M. Zanetti , E. V. Valetov , E. C. Dukes , R. Ehrlich , R. C. Group , J. Heeck , P. Q. Hung , S. M. Demers , G. Pezzullo , K. R. Lynch , J. L. Popp

The ALICE experiment is dedicated to the study of the quark gluon plasma in heavy-ion collisions at the CERN LHC. The Muon Forward Tracker (MFT) is under consideration by the ALICE experiment to be part of its program of detectors upgrade…

High Energy Physics - Experiment · Physics 2019-08-14 Antonio Uras

The Muon-to-Electron (Mu2e) experiment at Fermilab, will seek the evidence of direct muon to electron conversion at the sensitivity level where it cannot be explained by the Standard Model. An 8-GeV 25-kW proton beam will be directed onto a…

Accelerator Physics · Physics 2012-02-20 V. S. Pronskikh , V. V. Kashikhin , N. V. Mokhov

The Mu2e collaboration has proposed an experiment to search for the coherent, neutrino-less conversion of a muon into an electron in the Coulomb field of a nucleus with an expected sensitivity of $R_{\mu e}<6.0\times 10^{-17}$, at the 90%…

High Energy Physics - Experiment · Physics 2011-12-02 Robert K. Kutschke

There is a long standing discrepancy between the Standard Model prediction for the muon g-2 and the value measured by the Brookhaven E821 Experiment. At present the discrepancy stands at about three standard deviations, with a comparable…

Instrumentation and Detectors · Physics 2019-08-14 Graziano Venanzoni

The Muon g-2 Experiment (E989) at Fermilab is seeking to measure the anomalous magnetic moment of muon ($a_{\mu}$) with a precision of 140 parts-per-billion (ppb) and aiming to resolve the discrepancy between the E821 measurement and the…

Instrumentation and Detectors · Physics 2018-10-10 Ran Hong

The MuCool R&D program is described. The aim of MuCool is to develop all key pieces of hardware required for ionization cooling of a muon beam. This effort will lead to a more detailed understanding of the construction and operating costs…

Accelerator Physics · Physics 2019-08-14 Daniel M. Kaplan

The Muon g-2 experiment E989 at Fermilab measures the anomalous magnetic moment of the muon $a_\mu$ with improved precision compared to the Brookhaven (E821) experiments. The Brookhaven results are in tension with the Standard Model by more…

High Energy Physics - Experiment · Physics 2022-02-24 Alexander Tewsley-Booth