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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 Mu2e experiment at Fermilab will search for charged lepton flavor violation via the coherent conversion process mu- N --> e- N with a sensitivity approximately four orders of magnitude better than the current world's best limits for…

Instrumentation and Detectors · Physics 2015-03-18 L. Bartoszek , E. Barnes , J. P. Miller , J. Mott , A. Palladino , J. Quirk , B. L. Roberts , J. Crnkovic , V. Polychronakos , V. Tishchenko , P. Yamin , C. -h. Cheng , B. Echenard , K. Flood , D. G. Hitlin , J. H. Kim , T. S. Miyashita , F. C. Porter , M. Röhrken , J. Trevor , R. -Y. Zhu , E. Heckmaier , T. I. Kang , G. Lim , W. Molzon , Z. You , A. M. Artikov , J. A. Budagov , Yu. I. Davydov , V. V. Glagolev , A. V. Simonenko , Z. U. Usubov , S. H. Oh , C. Wang , G. Ambrosio , N. Andreev , D. Arnold , M. Ball , R. H. Bernstein , A. Bianchi , K. Biery , R. Bossert , M. Bowden , J. Brandt , G. Brown , H. Brown , M. Buehler , M. Campbell , S. Cheban , M. Chen , J. Coghill , R. Coleman , C. Crowley , A. Deshpande , G. Deuerling , J. Dey , N. Dhanaraj , M. Dinnon , S. Dixon , B. Drendel , N. Eddy , R. Evans , D. Evbota , J. Fagan , S. Feher , B. Fellenz , H. Friedsam , G. Gallo , A. Gaponenko , M. Gardner , S. Gaugel , K. Genser , G. Ginther , H. Glass , D. Glenzinski , D. Hahn , S. Hansen , B. Hartsell , S. Hays , J. A. Hocker , E. Huedem , D. Huffman , A. Ibrahim , C. Johnstone , V. Kashikhin , V. V. Kashikhin , P. Kasper , T. Kiper , D. Knapp , K. Knoepfel , L. Kokoska , M. Kozlovsky , G. Krafczyk , M. Kramp , S. Krave , K. Krempetz , R. K. Kutschke , R. Kwarciany , T. Lackowski , M. J. Lamm , M. Larwill , F. Leavell , D. Leeb , A. Leveling , D. Lincoln , V. Logashenko , V. Lombardo , M. L. Lopes , A. Makulski , A. Martinez , D. McArthur , F. McConologue , L. Michelotti , N. Mokhov , J. Morgan , A. Mukherjee , P. Murat , V. Nagaslaev , D. V. Neuffer , T. Nicol , J. Niehoff , J. Nogiec , M. Olson , D. Orris , R. Ostojic , T. Page , C. Park , T. Peterson , R. Pilipenko , A. Pla-Dalmau , V. Poloubotko , M. Popovic , E. Prebys , P. Prieto , V. Pronskikh , D. Pushka , R. Rabehl , R. E. Ray , R. Rechenmacher , R. Rivera , W. Robotham , P. Rubinov , V. L. Rusu , V. Scarpine , W. Schappert , D. Schoo , A. Stefanik , D. Still , Z. Tang , N. Tanovic , M. Tartaglia , G. Tassotto , D. Tinsley , R. S. Tschirhart , G. Vogel , R. Wagner , R. Wands , M. Wang , S. Werkema , H. B. White , J. Whitmore , R. Wielgos , R. Woods , C. Worel , R. Zifko , P. Ciambrone , F. Colao , M. Cordelli , G. Corradi , E. Dane , S. Giovannella , F. Happacher , A. Luca , S. Miscetti , B. Ponzio , G. Pileggi , A. Saputi , I. Sarra , R. S. Soleti , V. Stomaci , M. Martini , P. Fabbricatore , S. Farinon , R. Musenich , D. Alexander , A. Daniel , A. Empl , E. V. Hungerford , K. Lau , G. D. Gollin , C. Huang , D. Roderick , B. Trundy , D. Na. Brown , D. Ding , Yu. G. Kolomensky , M. J. Lee , M. Cascella , F. Grancagnolo , F. Ignatov , A. Innocente , A. L'Erario , A. Miccoli , A. Maffezzoli , P. Mazzotta , G. Onorato , G. M. Piacentino , S. Rella , F. Rossetti , M. Spedicato , G. Tassielli , A. Taurino , G. Zavarise , R. Hooper , D. No. Brown , R. Djilkibaev , V. Matushko , C. Ankenbrandt , S. Boi , A. Dychkant , D. Hedin , Z. Hodge , V. Khalatian , R. Majewski , L. Martin , U. Okafor , N. Pohlman , R. S. Riddel , A. Shellito , A. L. de Gouvea , F. Cervelli , R. Carosi , S. Di Falco , S. Donati , T. Lomtadze , G. Pezzullo , L. Ristori , F. Spinella , M. Jones , M. D. Corcoran , J. Orduna , D. Rivera , R. Bennett , O. Caretta , T. Davenne , C. Densham , P. Loveridge , J. Odell , R. Bomgardner , E. C. Dukes , R. Ehrlich , M. Frank , S. Goadhouse , R. Group , E. Ho , H. Ma , Y. Oksuzian , J. Purvis , Y. Wu , D. W. Hertzog , P. Kammel , K. R. Lynch , J. L. Popp

The Mu2e experiment searches for the neutrino-less muon to electron conversion in the field of a nucleus, which is a charged lepton flavor violating process. The goal of the experiment is to reach a single event sensitivity of 2.8 x…

Instrumentation and Detectors · Physics 2016-06-20 R. Donghia

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 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 2016-12-30 V. Pronskikh , D. Glenzinski , K. Knoepfel , N. Mokhov , R. Tschirhart

Mu2e at Fermilab will search for charged lepton flavor violation via the coherent conversion process mu- N --> e- N with a sensitivity approximately four orders of magnitude better than the current world's best limits for this process. The…

Instrumentation and Detectors · Physics 2012-12-06 The Mu2e Project , Collaboration , : , R. J. Abrams , D. Alezander , G. Ambrosio , N. Andreev , C. M. Ankenbrandt , D. M. Asner , D. Arnold , A. Artikov , E. Barnes , L. Bartoszek , R. H. Bernstein , K. Biery , V. Biliyar , R. Bonicalzi , R. Bossert , M. Bowden , J. Brandt , D. N. Brown , J. Budagov , M. Buehler , A. Burov , R. Carcagno , R. M. Carey , R. Carosi , M. Cascella , D. Cauz , F. Cervelli , A. Chandra , J. K. Chang , C. Cheng , P. Ciambrone , R. N. Coleman , M. Cooper , M. C. Corcoran , M. Cordelli , Y. Davydov , A. L. de Gouvea , L. De Lorenzis , P. T. Debevec , F. DeJongh , C. Densham , G. Deuerling , J. Dey , S. Di Falco , S. Dixon , R. Djilkibaev , B. Drendel , E. C. Dukes , A. Dychkant , B. Echenard , R. Ehrlich , N. Evans , D. Evbota , I. Fang , J. E. Fast , S. Feher , M. Fischler , M. Frank , E. Frlez , S. S. Fung , G. Gallo , G. Galucci , A. Gaponenko , K. Genser , S. Giovannella , V. Glagolev , D. Glenzinski , D. Gnani , S. Goadhouse , G. D. Gollin , C. Grace , F. Grancagnolo , C. Group , J. Hanson , S. Hanson , F. Happacher , E. Heckmaier , D. Hedin , D. W. Hertzog , R. Hirosky , D. G. Hitlin , E. Ho , X. Huang , E. Huedem , P. Q. Hung , E. V. Hungerford , T. Ito , W. Jaskierny , R. Jedziniak , R. P. Johnson , C. Johnstone , J. A. Johnstone , S. A. Kahn , P. Kammel , T. I. Kang , V. S. Kashikhin , V. V. Kashikhin , P. Kasper , D. M. Kawall , V. Khalatian , M. Kim , A. Klebaner , D. Kocen , Y. Kolomensky , I. Kourbanis , J. Kowalkowski , J. Kozminski , K. Krempetz , K. S. Kumar , R. K. Kutschke , R. Kwarciany , T. Lackowski , M. Lamm , M. Larwill , K. Lau , M. J. Lee , A. L'Erario , T. Leveling , G. Lim , C. Lindenmeyer , V. Logashenko , T. Lontadze , M. Lopes , A. Luca , K. R. Lynch , T. Ma , A. Maffezzoli , W. J. Marciano , M. Martini , W. Masayoshi , V. Matushko , M. McAteer , R. McCrady , A. Moccoli , L. Michelotti , J. P. Miller , S. Miscetti , W. Molzon , J. Morgan , A. Mukherjee , S. Nagaitsev , V. Nagaslaev , J. Niehoff , D. V. Neuffer , T. Nicol , A. J. Norman , B. Norris , J. Odell , S. Oh , Y. Oksuzian , G. Onorato , J. Orduna , D. Orris , R. Ostojic , T. Page , K. D. Paschke , G. Pauletta , T. Peterson , G. M. Piacentino , G. Pileggi , A. Pla-Dalmau , D. Pocanic , C. C. Polly , V. Polychronakos , B. Ponzio , M. Popovic , J. L. Popp , F. Porter , E. Presbys , P. Prieto , V. Pronskikh , F. Puccinelli , R. Rabehl , J. Ramsey , R. E. Ray , R. Rechenmacher , S. Rella , L. Ristori , R. Rivera , B. L. Roberts , T. J. Roberts , P. Rubinov , V. L. Rusu , A. Saputi , I. Sarra , Y. Smertzidis , P. Shanahan , A. Simonenko , J. Steward , I. Suslov , C. Sylvester , Z. Tang , M. Tartaglia , G. Tassielli , V. Tereshchenko , J. Theilacker , J. Tompkins , R. Tschirhart , G. Van Zandbergen , C. Vannini , G. Venanzoni , H. von der Lippe , R. Wagner , J. P. Walder , R. Walton , S. Wands , S. Wang , G. Warren , S. Werkema , H. B. White , R. Wielgos , L. S. Wood , M. Woodward , J. Wu , M. Xiao , R. Yamada , P. Yamin , K. Yarritu , K. Yonehara , C. Yoshikawa , Z. You , G. Yu , A. Yurkewicz , G. Zavarise , R. Y. Zhu

The Mu2e experiment will search for the neutrino-less conversion of a muon into an electron in the field of an aluminum nucleus. An observation would be the first signal of charged lepton flavor violation and de facto evidence for new…

High Energy Physics - Experiment · Physics 2020-07-15 Manolis Kargiantoulakis

The Mu2e Experiment at Fermilab will search for the coherent, neutrinoless conversion of muons into electrons in the field of an aluminium nucleus with an unprecedented sensitivity. Such a charged lepton flavor-violating reaction probes new…

High Energy Physics - Experiment · Physics 2016-09-08 Luca Morescalchi

The Mu2e experiment at Fermilab will search for the charged lepton flavor violating process of neutrino-less $\mu \to e$ coherent conversion in the field of an aluminum nucleus. About $7 \cdot 10^{17}$ muons, provided by a dedicated muon…

High Energy Physics - Experiment · Physics 2017-05-22 G. Pezzullo

The Mu2e experiment aims to test Charge Lepton Flavour Violation to an unprecedented level, enhancing the current sensitivity by four orders of magnitude for the neutrinoless conversion of muons into electrons. A series of graded solenoids…

Instrumentation and Detectors · Physics 2020-08-26 S. Giovannella

The Mu2e Experiment at Fermilab will search for coherent, neutrinoless conversion of muons into electrons in the field of a nucleus, with a sensitivity improvement of a factor of 10^4 over previous experiments. Such a charged lepton…

Instrumentation and Detectors · Physics 2019-08-12 Raffaella Donghia

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

The Mu2e experiment will search for a Standard Model violating rate of neutrinoless conversion of a muon into an electron in the presence of an aluminum nucleus. Observation of this charged lepton flavor violating process would be an…

High Energy Physics - Experiment · Physics 2022-10-28 Michael Thomas Hedges

The Mu2e experiment will search for the charged-lepton flavor violating (CLFV) neutrino-less conversion of a negative muon into an electron in the field of a nucleus. The conversion process results in a monochromatic electron with an energy…

Instrumentation and Detectors · Physics 2019-02-01 R. H. Bernstein

The use of existing Fermilab facilities to provide beams for two muon experiments -- the Muon to Electron Conversion Experiment (Mu2e) and the New g-2 Experiment -- is under consideration. Plans are being pursued to perform these…

Accelerator Physics · Physics 2009-10-20 M. J. Syphers

Since the discovery of the muon, particle physicists have carried out a series of experiments aimed at measuring flavor violation in charged-lepton interactions. To date, no such violation has been observed. The Mu2e experiment at Fermilab…

Instrumentation and Detectors · Physics 2014-01-20 Robert Craig Group , Yuri Oksuzian

The Mu2e experiment at Fermilab will search for the charged lepton flavour violating process of coherent neutrinoless muon-to-electron conversion in the presence of an aluminum nucleus. The muons are produced by an 8 GeV proton beam from…

Accelerator Physics · Physics 2025-09-29 Z. Liu , J. Williams , A. Makovec , M. Hedges , F. Pellemoine , K. Yonehara , G. Annala , K. Lynch , M. Bloomer , J. Popp , A. Edmonds , J. Miller

The Mu2e Experiment at Fermilab will search for coherent, neutrino-less conversion of negative muons into electrons in the field of an Aluminum nucleus, $\mu^- + Al \to e^- +Al$. Data collection start is planned for the end of 2021. The…

I describe the new generation of muon-to-electron conversion experiments, COMET and Mu2e, being constructed to make use of new high power pulsed muon beams a J-PARC and Fermilab respectively. A brief overview of the physics explored by the…

Instrumentation and Detectors · Physics 2014-12-04 R. P. Litchfield
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