The Mu2e experiment at Fermilab will search for the charged lepton flavor violating process of neutrino-less 𝜇→𝑒 μ → e coherent conversion in the field of an aluminum nucleus. Mu2e will reach a single event sensitivity of about 2.5⋅10−17 2.5 ⋅ 10 − 17 that corresponds to four orders of magnitude improvements with respect to the current best limit. The detector system consists of a straw tube tracker and a crystal calorimeter made of undoped CsI coupled with Silicon Photomultipliers. The calorimeter was designed to be operable in a harsh environment where about 10 krad/year will be delivered in the hottest region and work in presence of 1 T magnetic field. The calorimeter role is to perform 𝜇 μ /e separation to suppress cosmic muons mimiking the signal, while providing a high level trigger and a seeding the track search in the tracker. In this paper we present the calorimeter design and the latest R&D; results.

Design, status and perspective of the Mu2e crystal calorimeter

Martini M
2018-01-01

Abstract

The Mu2e experiment at Fermilab will search for the charged lepton flavor violating process of neutrino-less 𝜇→𝑒 μ → e coherent conversion in the field of an aluminum nucleus. Mu2e will reach a single event sensitivity of about 2.5⋅10−17 2.5 ⋅ 10 − 17 that corresponds to four orders of magnitude improvements with respect to the current best limit. The detector system consists of a straw tube tracker and a crystal calorimeter made of undoped CsI coupled with Silicon Photomultipliers. The calorimeter was designed to be operable in a harsh environment where about 10 krad/year will be delivered in the hottest region and work in presence of 1 T magnetic field. The calorimeter role is to perform 𝜇 μ /e separation to suppress cosmic muons mimiking the signal, while providing a high level trigger and a seeding the track search in the tracker. In this paper we present the calorimeter design and the latest R&D; results.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14241/4136
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