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Amsbaugh, J.F.; Barrett, J.; Beglarian, A.; Bergmann, T.; Bichsel, H.; Bodine, L.I.; Bonn, J.; Boyd, N.M.; Burritt, T.H.; Chaoui, Z.; Chilingaryan, S.; Corona, T.J.; Doe, P.J.; Dunmore, J.A.; Enomoto, S.; Formaggio, J.A.; Fränkle, F.M.; Furse, D.; Gemmeke, H.; Glück, F.; Harms, F.; Harper, G.C.; Hartmann, J.; Howe, M.A.; Kaboth, A.; Kelsey, J.; Knauer, M.; Kopmann, A.; Leber, M.L.; Martin, E.L.; Middleman, K.J.; Myers, A.W.; Oblath, N.S.; Parno, D.S.; Peterson, D.A.; Petzold, L.; Phillips, D.G.; Renschler, P.; Robertson, R.G.H.; Schwarz, J.; Steidl, M.; Tcherniakhovski, D.; Thümmler, T.; Van Wechel, T.D.; VanDevender, B.A.; Vöcking, S.; Wall, B.L.; Wierman, K.L.; Wilkerson, J.F.; Wüstling, S.
Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment, 04/2015, Letnik: 778, Številka: CJournal Article
The focal-plane detector system for the KArlsruhe TRItium Neutrino (KATRIN) experiment consists of a multi-pixel silicon p-i-n-diode array, custom readout electronics, two superconducting solenoid magnets, an ultra high-vacuum system, a high-vacuum system, calibration and monitoring devices, a scintillating veto, and a custom data-acquisition system. It is designed to detect the low-energy electrons selected by the KATRIN main spectrometer. We describe the system and summarize its performance after its final installation.
