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CCE measurments with A12 detectors in Ljubljana

CCE measurments with A12 detectors in Ljubljana. Alibava readout system, Kazu.ini settings Keithley 2410 HV unit 90 Sr source only detector cooled with Peltier element, not the readout chip Detectors: not irradiated: w639-bz3c-p15

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CCE measurments with A12 detectors in Ljubljana

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  1. CCE measurments with A12 detectors in Ljubljana • Alibavareadout system, Kazu.ini settings • Keithley 2410 HV unit • 90Sr source • only detector cooled with Peltier element, not the readout chip • Detectors: • not irradiated: w639-bz3c-p15 • 5e14 neutrons: w631-bz3c-p12 • 1e15 neutrons: w616-bz3c-p14 • 5e14 protons (B.): w627-bz3c-p2 • 1e15 protons (B.): w631-bz3c-p2 Igor Mandić, Jožef Stefan Institute, January 2014

  2. Setup PM Cooling block 90Sr source holder Detector Al support in thermal contact with cooling block Igor Mandić, Jožef Stefan Institute, January 2014

  3. Not irradiated • Cuts: • seed: 3.5 • neighbour: 1.8 • Fit: • convolution of • Gauss + Landau • Time distribution • select events between • 5 ns and 20 ns Igor Mandić, Jožef Stefan Institute, January 2014

  4. Not irradiated • three daughter boards  different gains • good agreement with Liverpool Igor Mandić, Jožef Stefan Institute, January 2014

  5. Neutrons • before annealing Ljubljana slightly higher than Liverpool • not much annealing • no difference between 80 minutes and 160 minutes at 60°C for 1e15 Igor Mandić, Jožef Stefan Institute, January 2014

  6. Protons (Birmingham)  detector irradiated to 5e14: very low charge (~ 3000 kel at 1000 V) • almost no annealing • at lower voltagesvery different from Liverpool • at lower voltages different than after neutron irradiation Igor Mandić, Jožef Stefan Institute, January 2014

  7. Comparison with A07 • A07 detectors measured with SCT128 setup •  good agreement after annealing Igor Mandić, Jožef Stefan Institute, January 2014

  8. Summary • A12 detectors irradiated to 5e14 and 1e15 with neutrons and Birmingham protons • measurements before controlled annealing and after 80 minutes at 60°C • neutrons: •  CCE increases max 10% after 80 minutes annealing  less than A07 detectors •  after annealing collected charge as in A07 detectors • protons: •  detector irradiated to 5e14 doesn’t work normally  charge too low: only about ~ 3 kel •  detector irradiated to 1e15: 80 minutes annealing has no effect •  charge vs. bias curve different than after neutron irradiation •  at lower voltages more charge after proton irradiation • Future work: • measure detectors irradiated to 2e15 and 5e15 with neutrons • measure detectors irradiated to 2e15 and 5e15 with 70 MeV protons at CYRIC Igor Mandić, Jožef Stefan Institute, January 2014

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