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  • Dead layer on silicon p–i–n...
    Wall, B.L.; Amsbaugh, J.F.; Beglarian, A.; Bergmann, T.; Bichsel, H.C.; Bodine, L.I.; Boyd, N.M.; Burritt, T.H.; Chaoui, Z.; Corona, T.J.; Doe, P.J.; Enomoto, S.; Harms, F.; Harper, G.C.; Howe, M.A.; Martin, E.L.; Parno, D.S.; Peterson, D.A.; Petzold, L.; Renschler, P.; Robertson, R.G.H.; Schwarz, J.; Steidl, M.; Van Wechel, T.D.; VanDevender, B.A.; Wüstling, S.; Wierman, K.J.; Wilkerson, J.F.

    Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment, 04/2014, Letnik: 744
    Journal Article

    Semiconductor detectors in general have a dead layer at their surfaces that is either a result of natural or induced passivation, or is formed during the process of making a contact. Charged particles passing through this region produce ionization that is incompletely collected and recorded, which leads to departures from the ideal in both energy deposition and resolution. The silicon p-i-n diode used in the KATRIN neutrino-mass experiment has such a dead layer. We have constructed a detailed Monte Carlo model for the passage of electrons from vacuum into a silicon detector, and compared the measured energy spectra to the predicted ones for a range of energies from 12 to 20 keV. The comparison provides experimental evidence that a substantial fraction of the ionization produced in the "dead" layer evidently escapes by diffusion, with 46% being collected in the depletion zone and the balance being neutralized at the contact or by bulk recombination. The most elementary model of a thinner dead layer from which no charge is collected is strongly disfavored.