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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

In a few years, the COMET experiment at J-PARC and the Mu2e experiment at Fermilab will probe the $\mu-e$ conversion rate in the vicinity of $\mathcal{O}(10^{-17})$ for an Al target with high experimental sensitivity. Within the framework…

High Energy Physics - Phenomenology · Physics 2022-08-16 Ze-Ning Zhang , Hai-Bin Zhang , Xing-Xing Dong , Jin-Lei Yang , Wei Li , Zhong-Jun Yang , Tong-Tong Wang , Tai-Fu Feng

The Mu2e experiment at Fermilab aims to measure the charged lepton flavor violating neutrinoless muon to electron conversion. The goal of the experiment is to reach a single event sensitivity of 2.5 x 10^{-17}, to set an upper limit on the…

Instrumentation and Detectors · Physics 2016-11-23 Raffaella Donghia

The Mu2e experiment at Fermilab aims at measuring the neutrinoless conversion of a negative muon into an electron and reach a single event sensitivity of 2.5x10^{-17} after three years of data taking. The monoenergetic electron produced in…

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 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. Mu2e will reach a single event sensitivity of about $2.5\cdot…

The Mu2e and COMET experiments are expected to improve existing limits on charged lepton flavor violation (CLFV) by roughly four orders of magnitude. $\mu\rightarrow e$ conversion experiments are typically optimized for electrons produced…

High Energy Physics - Phenomenology · Physics 2025-01-08 W. C. Haxton , Evan Rule

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

Mu2e and COMET will search for electrons produced via the neutrinoless conversion of stopped muons bound in 1s atomic orbits of $^{27}$Al, improving existing limits on charged lepton flavor violation (CLFV) by roughly four orders of…

High Energy Physics - Phenomenology · Physics 2024-09-18 W. C. Haxton , Evan Rule

The upcoming Mu3e experiment searches for the lepton flavour violating decay $\mu^+\,\rightarrow\,e^+ e^- e^+$ with the aim of a final sensitivity of one signal decay in $10^{16}$ observed muon decays, an improvement over the preceding…

Instrumentation and Detectors · Physics 2018-02-28 Ann-Kathrin Perrevoort

The Mu2e experiment at Fermilab will search for the neutrinoless $\mu^- \to e^-$ conversion in the field of an aluminum nucleus. The Mu2e data-taking plan assumes two running periods, Run I and Run II, separated by an approximately…

High Energy Physics - Experiment · Physics 2022-10-21 Mu2e Collaboration

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

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

The upcoming Mu3e experiment aims to search for the lepton flavour violating decay $\mu^+ \to e^+ e^- e^+$ with an unprecedented final sensitivity of one signal decay in $10^{16}$ observed muon decays by making use of an innovative…

High Energy Physics - Experiment · Physics 2018-12-04 Ann-Kathrin Perrevoort

Mu3e is an experiment currently under construction at the Paul Scherrer Institute in Switzerland, designed to search for the Lepton Flavor Violating (LFV) decay $\mu^+ \rightarrow e^+e^-e^+$. In extensions of the Standard Model (SM) that…

High Energy Physics - Experiment · Physics 2025-01-27 Robert Mihai Amarinei

We report on the status of charged lepton flavor violating (CLFV) experiments with muons. We focus on the three "golden channels": $\mu^{+} \rightarrow e^{+} \gamma$, $\mu^{+} \rightarrow e^{+} e^{-} e^{+}$ and $\mu^{-} N \rightarrow e^{-}…

High Energy Physics - Experiment · Physics 2025-05-09 Dylan Palo

The Mu2e experiment at Fermilab will search for Charged Lepton Flavor Violating conversion of a muon to an electron in an atomic field. The Mu2e detector is composed of a tracker, an electromagnetic calorimeter and an external system,…

The Mu2e experiment will search for coherent, neutrino-less conversion of muons into electrons in the Coulomb field of an aluminum nucleus with a sensitivity of four orders of magnitude better than previous experiments. The signature of…

Instrumentation and Detectors · Physics 2017-10-12 Alessandra Lucà

The observation of lepton flavour violation (LFV) in the charged lepton sector would be an unambiguous sign of physics beyond the Standard Model (BSM), and thus, it is the channel of choice for many BSM searches. LFV searches in muon decays…

High Energy Physics - Experiment · Physics 2023-08-23 Ann-Kathrin Perrevoort