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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 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 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 muon-to-electron conversion (Mu2e) experiment at Fermilab will be used to search for the charged lepton flavor-violating conversion of muons to electrons in the field of an atomic nucleus. The Mu2e experiment is currently 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

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

The Muon-to-Electron Conversion (Mu2e) Experiment demands a highly precise magnet and collimator system to achieve a stringent extinction level of $1\times 10^{-10}$ for out-of-time beam particles. Extinction is ensured by an AC Dipole…

Accelerator Physics · Physics 2024-05-09 Ryan Hensley , Eric Prebys , Sridhar Tripathy

We report on several versions of the calibration and monitoring system dedicated to scintillator tile calorimeters built within the CALICE collaboration and intended for future linear collider experiments. Whereas the first, a 1 m3 analogue…

Instrumentation and Detectors · Physics 2019-08-15 Jaroslav Zalesak

We report the test of many of the key elements of the laser-based calibration system for muon g - 2 experiment E989 at Fermilab. The test was performed at the Laboratori Nazionali di Frascati's Beam Test Facility using a 450 MeV electron…

The Muon Campus at Fermilab provides world class accelerator infrastructure supporting the next generation intensity frontier experiments. The anti-proton source from the Tevatron era was converted to the present day Muon Campus at the end…

Accelerator Physics · Physics 2022-08-08 S. Ganguly

The new muon (g-2) experiment E989 at Fermilab will be equipped with a laser calibration system for all the 1296 channels of the calorimeters. An integrating sphere and an alternative system based on an engineered diffuser have been…

The motivation of the current R&D project is based upon the requirements of the JEDI international collaboration aiming to measure Electric Dipole Moments (EDMs) of charged particles in storage rings. One of the most important elements of…

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 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 DarkSide-20k dark matter direct detection experiment will employ a 21 m^2 silicon photomultiplier (SiPM) array, instrumenting a dual-phase 50 tonnes liquid argon Time Projection Chamber (TPC). SiPMs are arranged into modular…

Instrumentation and Detectors · Physics 2025-07-11 F. Acerbi , P. Adhikari , P. Agnes , I. Ahmad , S. Albergo , I. F. Albuquerque , T. Alexander , A. K. Alton , P. Amaudruz , M. Angiolilli , E. Aprile , M. Atzori Corona , D. J. Auty , M. Ave , I. C. Avetisov , O. Azzolini , H. O. Back , Z. Balmforth , A. Barrado Olmedo , P. Barrillon , G. Batignani , P. Bhowmick , M. Bloem , S. Blua , V. Bocci , W. Bonivento , B. Bottino , M. G. Boulay , T. Braun , A. Buchowicz , S. Bussino , J. Busto , M. Cadeddu , M. Cadoni , R. Calabrese , V. Camillo , A. Caminata , N. Canci , M. Caravati , M. Cárdenas-Montes , N. Cargioli , M. Carlini , A. Castellani , P. Cavalcante , S. Cebrian , S. Chashin , A. Chepurnov , S. Choudhary , L. Cifarelli , B. Cleveland , Y. Coadou , V. Cocco , D. Colaiuda , E. Conde Vilda , L. Consiglio , A. F. V. Cortez , B. S. Costa , M. Czubak , M. D'Aniello , S. D'Auria , M. D. Da Rocha Rolo , A. Dainty , G. Darbo , S. Davini , R. de Asmundis , S. De Cecco , G. Dellacasa , A. V. Derbin , A. Devoto , L. Di Noto , P. Di Stefano , L. K. Dias , D. Díaz Mairena , C. Dionisi , G. Dolganov , F. Dordei , V. Dronik , F. Dylon , A. Elersich , E. Ellingwood , T. Erjavec , N. Fearon , M. Fernandez Diaz , L. Ferro A. Ficorella , G. Fiorillo , D. Fleming , P. Franchini , D. Franco , H. Frandini Gatti , E. Frolov , F. Gabriele , D. Gahan , C. Galbiati , G. Galiński , G. Gallina , M. Garbini , P. Garcia Abia , A. Gawdzik , A. Gendotti , G. K. Giovanetti , V. Goicoechea Casanueva , A. Gola , L. Grandi , G. Grauso , G. Grilli di Cortona , A. Grobov , M. Gromov , M. Gulino , B. R. Hackett , A. L. Hallin , A. Hamer , M. Haranczyk , B. Harrop , T. Hessel , C. Hidalgo , J. Hollingham , S. Horikawa , J. Hu , F. Hubaut , D. Huff , T. Hugues , E. V. Hungerford , A. Ianni , A. Ianni , V. Ippolito , A. Jamil , C. Jillings , R. Keloth , N. Kemmerich , A. Kemp , M. Kimura , A. Klenin , K. Kondo , G. Korga , L. Kotsiopoulou , S. Koulosousas , A. Kubankin , P. Kunzé , M. Kuss , M. Kuźniak , M. Kuzwa , M. La Commara , M. Lai , E. Le Guirriec , E. Leason , A. Leoni , L. Lidey , J. Lipp , M. Lissia , L. Luzzi , O. Lychagina , O. Macfadyen , I. Machts , I. N. Machulin , S. Manecki , I. Manthos , L. Mapelli , A. Marasciulli , S. M. Mari , C. Mariani , J. Maricic , M. Martinez , C. J. Martoff , G. Matteucci , K. Mavrokoridis , A. B. McDonald , S. Merzi , A. Messina , R. Milincic , S. Minutoli , A. Mitra , J. Monroe , E. Moretti , M. Morrocchi , A. Morsy , T. Mroz , V. N. Muratova , M. Murra , P. Musico , R. Nania , M. Nessi , G. Nieradka , K. Nikolopoulos , E. Nikoloudaki , I. Nikulin , J. Nowak , K. Olchanski , A. Oleinik , V. Oleynikov , P. Organtini , A. Ortiz de Solórzano , A. Padmanabhan , M. Pallavicini , L. Pandola , E. Pantic , E. Paoloni , D. Papi , B. Park , G. Pastuszak , G. Paternoster , R. Pavarani , A. Peck , K. Pelczar , R. Perez , V. Pesudo , S. Piacentini , N. Pino , G. Plante , A. Pocar , S. Pordes , P. Pralavorio , E. Preosti , D. Price , M. Pronesti , S. Puglia , M. Queiroga Bazetto , F. Raffaelli , F. Ragusa , Y. Ramachers , A. Ramirez , S. Ravinthiran , M. Razeti , A. L. Renshaw , A. Repond , M. Rescigno , S. Resconi , F. Retiere , L. P. Rignanese , A. Ritchie-Yates , A. Rivetti , A. Roberts , C. Roberts , G. Rogers , L. Romero , M. Rossi , A. Rubbia , D. Rudik , J. Runge , M. A. Sabia , P. Salomone , O. Samoylov , S. Sanfilippo , D. Santone , R. Santorelli , E. M. Santos , I. Sargeant , C. Savarese , E. Scapparone , F. G. Schuckman , G. Scioli , D. A. Semenov , M. Sestu , V. Shalamova , S. Sharma Poudel , A. Sheshukov , M. Simeone , P. Skensved , M. D. Skorokhvatov , O. Smirnov , T. Smirnova , B. Smith , F. Spadoni , M. Spangenberg , A. Steri , V. Stornelli , S. Stracka , A. Sung , C. Sunny , Y. Suvorov , A. M. Szelc , O. Taborda , R. Tartaglia , A. Taylor , J. Taylor , G. Testera , K. Thieme , A. Thompson , S. Torres-Lara , A. Tricomi , S. Tullio , E. V. Unzhakov , M. Van Uffelen , P. Ventura , T. Viant , S. Viel , A. Vishneva , R. B. Vogelaar , J. Vossebeld , B. Vyas , M. Wada , M. Walczak , Y. Wang , S. Westerdale , L. Williams , M. M. Wojcik , M. Wojcik , C. Yang , J. Yin A. Zabihi , P. Zakhary , A. Zani , Y. Zhang , T. Zhu , A. Zichichi , G. Zuzel , M. P. Zykova

With the successful construction and operation of a highly granular hadron calorimeter system, featuring approx. 22000 individually read out SiPM-on-tile channels, the CALICE collaboration has set the next milestone in proving the…

Instrumentation and Detectors · Physics 2022-11-09 Daniel Heuchel

Silicon Photomultipliers (SiPM) represent a promising alternative to classical photomultipliers, for instance, for the detection of photons in high energy physics and medical physics. In the present work, electrical characterizations of…

Instrumentation and Detectors · Physics 2017-08-23 M. J. Boschini , C. Consolandi , P. G. Fallica , M. Gervasi , D. Grandi , M. Mazzillo , S. Pensotti , P. G. Rancoita , D. Sanfilippo , M. Tacconi , G. Valvo

The event plane detector (EPD), installed in the Solenoid Tracker at the Relativistic Heavy-Ion Collider located at the Brookhaven National Laboratory is a plastic scintillator-based device that measures the reaction centrality and event…

Instrumentation and Detectors · Physics 2020-11-24 Ming Shao , Yitao Wu , Zheng Liang , Kaifeng Shen , Zebo Tang , M. A. Lisa , R. Reed , G. Visser , Yongjie Sun , Yi Zhou , Jian Zhou , Guofeng Song , Dongdong Hu , Xu Wang , Xinjian Wang

Silicon photomultipliers (SiPMs) will be used to read out all calorimeters in the ePIC experiment at the Electron-Ion Collider (EIC). A thorough characterization of the radiation damage expected for SiPMs under anticipated EIC fluences is…

Instrumentation and Detectors · Physics 2025-06-23 Jiajun Huang , Sean Preins , Ryan Tsiao , Miguel Rodriguez , Barak Schmookler , Miguel Arratia

Sufficient energy resolution is the key issue for the calorimetry in particle and nuclear physics. The calorimeter of the A4 parity violation experiment at MAMI is a segmented calorimeter where the energy of an event is determined by…