Silicon Photomultipliers for the decay tunnel instrumentation of the ENUBET neutrino beam
- Pozzato M.
- Acerbi F.
- Ballerini G.
- Berra A.
- Bonesini M.
- Branca A.
- Brizzolari C.
- Brunetti G.
- Calviani M.
- Capelli S.
- Carturan S.
- Catanesi M. G.
- Cecchini S.
- Charitonidis N.
- Cindolo F.
- Collazuol G.
- Conti E.
- Corso F. D.
- Delogu C.
- De Rosa G.
- Falcone A.
- Gola A.
- Jollet C.
- Kain V.
- Klicek B.
- Kudenko Y.
- Laveder M.
- Longhin A.
- Ludovici L.
- Lutsenko E.
- Magaletti L.
- Mandrioli G.
- Margotti A.
- Mascagna V.
- Mauri N.
- Meazza L.
- Meregaglia A.
- Mezzetto M.
- Nessi M.
- Paoloni A.
- Pari M.
- Parozzi E. G.
- Pasqualini L.
- Paternoster G.
- Patrizii L.
- Prest M.
- Pupilli F.
- Radicioni E.
- Riccio C.
- Ruggieri A. C.
- Scian C.
- Sirri G.
- Soldani M.
- Stipcevic M.
- Tenti M.
- Terranova F.
- Torti M.
- Vallazza E.
- Velotti F.
- Vesco M.
- Votano L.
DOIAbstract
The goal of the ENUBET project is to demonstrate that a precision of ∼1% on measurement of the absolute neutrino cross section at GeV scale can be achieved by monitoring the positron production in the decay tunnel coming from the three-body semileptonic decays of kaons. The baseline option for the tunnel instrumentation employs a fine-grained shashlik calorimeter with a 4.3 X0 longitudinal segmentation to separate positrons and pions coming from other decay modes of kaons. The system is complemented by rings of plastic scintillator doublets below the calorimeter acting as a photon veto to suppress the π0 background and to provide timing informations. SiPMs instrumenting the detector will be exposed to sizeble amounts of neutrons arising in ...
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