The Mu2e Crystal Calorimeter: An Overview

The Mu2e experiment at Fermilab will search for the standard model-forbidden, charged lepton flavour-violating conversion of a negative muon into an electron in the field of an aluminium nucleus. The distinctive signal signature is represented by a mono-energetic electron with an energy near the muo...

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Veröffentlicht in:Instruments (Basel) 2022-10, Vol.6 (4), p.60
Hauptverfasser: Atanov, Nikolay, Baranov, Vladimir, Borrel, Leo, Bloise, Caterina, Budagov, Julian, Ceravolo, Sergio, Cervelli, Franco, Colao, Francesco, Cordelli, Marco, Corradi, Giovanni, Davydov, Yuri, Falco, Stefano Di, Diociaiuti, Eleonora, Donati, Simone, Echenard, Bertrand, Ferrari, Carlo, Gioiosa, Antonio, Giovannella, Simona, Giusti, Valerio, Glagolev, Vladimir, Grancagnolo, Francesco, Hampai, Dariush, Happacher, Fabio, Hitlin, David, Martini, Matteo, Middleton, Sophie, Miscetti, Stefano, Morescalchi, Luca, Paesani, Daniele, Pasciuto, Daniele, Pedreschi, Elena, Porter, Frank, Raffaelli, Fabrizio, Saputi, Alessandro, Sarra, Ivano, Spinella, Franco, Taffara, Alessandra, Zanetti, Anna Maria, Zhu, Ren Yuan
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Sprache:eng
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Zusammenfassung:The Mu2e experiment at Fermilab will search for the standard model-forbidden, charged lepton flavour-violating conversion of a negative muon into an electron in the field of an aluminium nucleus. The distinctive signal signature is represented by a mono-energetic electron with an energy near the muon’s rest mass. The experiment aims to improve the current single-event sensitivity by four orders of magnitude by means of a high-intensity pulsed muon beam and a high-precision tracking system. The electromagnetic calorimeter complements the tracker by providing high rejection power in muon to electron identification and a seed for track reconstruction while working in vacuum in presence of a 1 T axial magnetic field and in a harsh radiation environment. For 100 MeV electrons, the calorimeter should achieve: (a) a time resolution better than 0.5 ns, (b) an energy resolution
ISSN:2410-390X
2410-390X
DOI:10.3390/instruments6040060