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The MUonE experiment proposes a novel approach to determine the leading hadronic contribution to the muon g-2, from a precise measurement of the differential cross section of the $\mu-e$ elastic scattering, achievable by using the CERN SPS…

High Energy Physics - Experiment · Physics 2024-01-09 E. Spedicato

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 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

A single calorimeter station for the Muon $g-2$ experiment at Fermilab includes the following subsystems: a 54-element array of PbF$_{2}$ Cherenkov crystals read out by large-area SiPMs, bias and slow-control electronics, a suite of 800…

We have developed a custom amplifier board coupled to a large-format 16-channel Hamamatsu silicon photomultiplier device for use as the light sensor for the electromagnetic calorimeters in the Muon g-2 experiment at Fermilab. The…

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

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 calorimeter is composed of 1400 un-doped CsI crystals, coupled to large area UV extended Silicon Photomultipliers (SiPMs), arranged in two annular disks. This calorimeter has to provide precise information on energy, timing and…

Instrumentation and Detectors · Physics 2017-03-08 S. Baccaro , A. Cemmi , M. Cordelli , E. Diociaiuti , R. Donghia , A. Ferrari , S. Giovannella , S. Miscetti , S. Müller , M. Pillon , I. Sarra

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 cosmic ray veto detector for the Mu2e experiment consists of scintillation bars embedded with wavelength-shifting fibers and read out by silicon photomultipliers (SiPMs). In this manuscript the calibration procedures of the SiPMs are…

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

Since the first version of the Mu2e TDR released at the beginning of 2015, the Mu2e Calorimeter system has undergone a long list of changes to arrive to its final design. These changes were primarily caused by two reasons: (i) the…

The electromagnetic calorimeter for the new muon (g-2) experiment at Fermilab will consist of arrays of PbF2 Cherenkov crystals read out by large-area silicon photo-multiplier (SiPM) sensors. We report here on measurements and simulations…

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 at Fermilab will search for the charged-lepton flavor-violating process of a neutrino less muon-to-electron decay in the presence of a nucleus. The experiment expects a single-event sensitivity of $2.9\times10^{-17}$,…

Instrumentation and Detectors · Physics 2019-10-03 Hannah Woodward

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

Scintillation properties of pure CsI crystals used in the shower calorimeter being built for precise determination of the pi+ -> pi0 e+ nu decay rate are reported. Seventy-four individual crystals, polished and wrapped in Teflon foil, were…

High Energy Physics - Experiment · Physics 2009-10-31 E. Frlez , I. Supek , K. A. Assamagan , Ch. Br"onnimann , Th. Fl"ugel , B. Krause , D. W. Lawrence , D. Mzavia , D. Pocanic , D. Renker , S. Ritt , P. L. Slocum , N. Soic

The Mu2e experiment, under construction at Fermilab, will search for the neutrino-less coherent $\mu^-N\rightarrow e^-N$ conversion in the field of a $^{27}$Al nucleus. Such a process violates lepton flavor conservation. About $60\%$ of…

Instrumentation and Detectors · Physics 2025-01-13 Alessandro Maria Ricci

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