Characterisation of the Hamamatsu photomultipliers for the KM3NeT Neutrino Telescope

The Hamamatsu R12199-02 3-inch photomultiplier tube is the photodetector chosen for the first phase of the KM3NeT neutrino telescope. About 7000 photomultipliers have been characterised for dark count rate, timing spread and spurious pulses. The quantum efficiency, the gain and the peak-to-valley ra...

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Veröffentlicht in:JINST 2018-05, Vol.13 (5), p.P05035-P05035
Hauptverfasser: Aiello, S., Akrame, S.E., Ameli, F., Anassontzis, E. G., Andre, M., Androulakis, G., Anghinolfi, M., Anton, G., Ardid, M., Aublin, J., Avgitas, T., Baars, M., Bagatelas, C., Barbarino, G., Baret, B., Barrios-Martí, J., Belias, A., Berbee, E., Berg, A. van den, Bertin, V., Biagi, S., Biagioni, A., Biernoth, C., Bormuth, R., Boumaaza, J., Bourret, S., Bouwhuis, M., Bozza, C., Brânzaş, H., Briukhanova, N., Bruijn, R., Brunner, J., Buis, E., Buompane, R., Busto, J., Calvo, D., Capone, A., Caramete, L., Celli, S., Chabab, M., Cherubini, S., Chiarella, V., Chiarusi, T., Circella, M., Cocimano, R., Coelho, J.A.B., Coleiro, A., Molla, M. Colomer, Coniglione, R., Coyle, P., Creusot, A., Cuttone, G., D'Onofrio, A., Dallier, R., Sio, C. De, Palma, I. Di, Díaz, A.F., Distefano, C., Domi, A., Donà, R., Donzaud, C., Dornic, D., Dörr, M., Durocher, M., Eberl, T., Eijk, D. van, Bojaddaini, I. El, Elsaesser, D., Enzenhöfer, A., Ferrara, G., Fusco, L.A., Gal, T., Garufi, F., Gauchery, S., Geißelsöder, S., Gialanella, L., Giorgio, E., Giuliante, A., Gozzini, S.R., Ruiz, R. Gracia, Graf, K., Grasso, D., Grégoire, T., Grella, G., Hallmann, S., Haren, H. van, Heid, T., Heijboer, A., Hekalo, A., Hernández-Rey, J.J., Hofestädt, J., Illuminati, G., James, C.W., Jongen, M., Jongewaard, B., de Jong, M., de Jong, P., Kadler, M., Kalaczyński, P., Kalekin, O.
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Sprache:eng
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Zusammenfassung:The Hamamatsu R12199-02 3-inch photomultiplier tube is the photodetector chosen for the first phase of the KM3NeT neutrino telescope. About 7000 photomultipliers have been characterised for dark count rate, timing spread and spurious pulses. The quantum efficiency, the gain and the peak-to-valley ratio have also been measured for a sub-sample in order to determine parameter values needed as input to numerical simulations of the detector.
ISSN:1748-0221
1748-0221
DOI:10.1088/1748-0221/13/05/P05035