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  • Technical design of the pha...
    Arndt, K.; Augustin, H.; Baesso, P.; Berger, N.; Berg, F.; Betancourt, C.; Bortoletto, D.; Bravar, A.; Briggl, K.; vom Bruch, D.; Buonaura, A.; Cadoux, F.; Chavez Barajas, C.; Chen, H.; Cooke, P.; Corrodi, S.; Damyanova, A.; Demets, Y.; Dittmeier, S.; Eckert, P.; Ehrler, F.; Fahrni, D.; Gagneur, S.; Gerritzen, L.; Goldstein, J.; Gottschalk, D.; Grab, C.; Gredig, R.; Groves, A.; Hammerich, J.; Hartenstein, U.; Hartmann, U.; Hayward, H.; Herkert, A.; Hetzel, S.; Hildebrandt, M.; Hodge, Z.; Hofer, A.; Huang, Q.H.; Hughes, S.; Huth, L.; Immig, D.M.; Jones, T.; Jones, M.; Kästli, H.-C.; Köppel, M.; Kettle, P.-R.; Kiehn, M.; Kilani, S.; Klingenmeyer, H.; Knecht, A.; Knight, A.; Kotlinski, B.; Kozlinskiy, A.; Lockwood, G.; Loreti, A.; La Marra, D.; Müller, M.; Meier, B.; Meier Aeschbacher, F.; Meneses, A.; Metodiev, K.; Mtchedlishvili, A.; Muley, S.; Munwes, Y.; Noehte, L.O.S.; Owen, P.; Papa, A.; Paraskevas, I.; Perić, I.; Perrevoort, A.-K.; Plackett, R.; Pohl, M.; Ritt, S.; Robmann, P.; Rompotis, N.; Rudzki, T.; Rutar, G.; Schöning, A.; Schimassek, R.; Schultz-Coulon, H.-C.; Serra, N.; Shen, W.; Shipsey, I.; Shrestha, S.; Steinkamp, O.; Stoykov, A.; Straumann, U.; Streuli, S.; Stumpf, K.; Tata, N.; Velthuis, J.; Vigani, L.; Vilella-Figueras, E.; Vossebeld, J.; Wasili, A.; Wauters, F.; Wiedner, D.; Windelband, B.; Zhong, T.

    Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment, 10/2021, Letnik: 1014
    Journal Article

    The Mu3e experiment aims to find or exclude the lepton flavour violating decay μ→eee at branching fractions above 10−16. A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of 2⋅10−15. We present an overview of all aspects of the technical design and expected performance of the phase I Mu3e detector. The high rate of up to 108 muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements.