N. Atanov, V. Baranov, L. Borrel, C. Bloise, J. Budagov, S. Ceravolo, F. Cervelli, F. Colao, M. Cordelli, G. Corradi, Y. Davydov, S. Falco, E. Diociaiuti, S. Donati, B. Echenard, C. Ferrari, A. Gioiosa, S. Giovannella, V. Giusti, V. Glagolev, F. Grancagnolo, D. Hampai, F. Happacher, D. Hitlin, M. Martini, S. Middleton, S. Miscetti, L. Morescalchi, D. Paesani, D. Pasciuto, E. Pedreschi, F. Porter, F. Raffaelli, A. Saputi, I. Sarra, F. Spinella, A. Taffara, A. Zanetti, R. Zhu
{"title":"The Mu2e Crystal Calorimeter: An Overview","authors":"N. Atanov, V. Baranov, L. Borrel, C. Bloise, J. Budagov, S. Ceravolo, F. Cervelli, F. Colao, M. Cordelli, G. Corradi, Y. Davydov, S. Falco, E. Diociaiuti, S. Donati, B. Echenard, C. Ferrari, A. Gioiosa, S. Giovannella, V. Giusti, V. Glagolev, F. Grancagnolo, D. Hampai, F. Happacher, D. Hitlin, M. Martini, S. Middleton, S. Miscetti, L. Morescalchi, D. Paesani, D. Pasciuto, E. Pedreschi, F. Porter, F. Raffaelli, A. Saputi, I. Sarra, F. Spinella, A. Taffara, A. Zanetti, R. Zhu","doi":"10.3390/instruments6040060","DOIUrl":null,"url":null,"abstract":"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 <10%, and (c) a position resolution of 1 cm. The calorimeter design consists of two disks, each loaded with 674 undoped CsI crystals read out by two large-area arrays of UV-extended SiPMs and custom analogue and digital electronics. We describe here the status of construction for all calorimeter components and the performance measurements conducted on the large-sized prototype with electron beams and minimum ionizing particles at a cosmic ray test stand. A discussion of the calorimeter’s engineering aspects and the on-going assembly is also reported.","PeriodicalId":13582,"journal":{"name":"Instruments","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2022-10-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Instruments","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.3390/instruments6040060","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"Physics and Astronomy","Score":null,"Total":0}
引用次数: 2
Abstract
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 <10%, and (c) a position resolution of 1 cm. The calorimeter design consists of two disks, each loaded with 674 undoped CsI crystals read out by two large-area arrays of UV-extended SiPMs and custom analogue and digital electronics. We describe here the status of construction for all calorimeter components and the performance measurements conducted on the large-sized prototype with electron beams and minimum ionizing particles at a cosmic ray test stand. A discussion of the calorimeter’s engineering aspects and the on-going assembly is also reported.