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a design study for a cobra upgrade to - Institut für Kern- und ...

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60 5 Scintilla<strong>to</strong>r <strong>upgrade</strong><br />

three different PMTs, one PIN diode, one APD and two Si-PMT. The<br />

implemented PMTs correspond <strong>to</strong> Hamamatsu R669 (borosilicate window,<br />

extended red pho<strong>to</strong>cathode), R6094 (borosilicate window and<br />

bialkali pho<strong>to</strong>cathode) and a R5900 with UV Glass and multialkali<br />

pho<strong>to</strong> cathode. The PIN diode is a 2x1 cm 2 S2744-08, the APD a S8664-<br />

1010 (10x10 mm 2 ) and the Si-PMT correspond <strong>to</strong> S10985-050C (MPPC-<br />

050C) with 6x6 mm 2 active area and four times 900 pixels and the<br />

S10985-100C (MPPC-100C) with four times 3600 pixels.<br />

Figure 5.2: Quantum efficiencies <strong>for</strong> pho<strong>to</strong> absorption of various electronic<br />

readouts in comparison <strong>to</strong> CsI:Tl emission spectrum [41].<br />

In this application, the default geometry can be changed with messengers,<br />

redefining the crystal size, the amount of placed readout devices<br />

and the size of the readout devices. Also, optical properties, like<br />

the housing finish of the crystal surface can be set <strong>to</strong> polished with<br />

the parameter ID (1), polished-frontpainted (2), polished-backpainted<br />

(3), gro<strong>und</strong> (4), gro<strong>und</strong>-frontpainted (5) and gro<strong>und</strong>-backpainted (6).<br />

Available quantum efficiencies are these of the PMT R669 (1), the PMT<br />

R6094 (2), the APD (3), the MPPC-100C (4), the MPPC-050C (5), the PIN<br />

diode (6) and the PMT R5900 (7). These parameters can be changed by<br />

using these commands:<br />

/CsI/detec<strong>to</strong>r/dimensions 20.00 5.00 5.00 cm<br />

/CsI/detec<strong>to</strong>r/pmtRadius 2.5 mm<br />

/CsI/detec<strong>to</strong>r/nx 0

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