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

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62 5 Scintilla<strong>to</strong>r <strong>upgrade</strong><br />

vice. The length of the light guide depends on the number of devices<br />

and the readout size. A visualisation, using the visualisation system<br />

Heprep, is shown in fig. 5.3.<br />

With this developed Geant4 application, different aspects of the scintillation<br />

detec<strong>to</strong>r preparation were studied.<br />

DATA ANALYSIS<br />

Be<strong>for</strong>e starting the comparison between the readout devices, the influence<br />

of the housing finish, reflectivity and absorption length was studied.<br />

There<strong>for</strong>e all 6 different kinds of housing finish were simulated<br />

with a PMT readout, covering the front faces of the crystal. The finish<br />

”polished” yields highest amount of pho<strong>to</strong> electrons. Gro<strong>und</strong>, gro<strong>und</strong>and<br />

polished-frontpainted yield aro<strong>und</strong> 75 % of the previous amount<br />

of pho<strong>to</strong> electrons. The gro<strong>und</strong>- and polished-backpainted finish only<br />

aro<strong>und</strong> 60 % of the pho<strong>to</strong> electron yield, obtained with a polished surface.<br />

The influence of the surface finish on the uni<strong>for</strong>mity of the signal <strong>for</strong><br />

different source positions was not studied, but a higher uni<strong>for</strong>mity of<br />

light collection <strong>for</strong> gro<strong>und</strong>, than <strong>for</strong> polished surfaces is expected [29].<br />

The further simulations were carried out with a gro<strong>und</strong> surface finish<br />

and a reflectivity of 0.98.<br />

As main examination, the amount of pho<strong>to</strong> electrons detected by different<br />

readout devices was evaluated. There<strong>for</strong>e these 7 readout devices<br />

were simulated with different sizes of active area. In a first simulation,<br />

the readout devices covered the entire front facing crystal side, in<br />

another simulation, only commercially available sizes <strong>for</strong> the readout<br />

devices were taken in<strong>to</strong> account. 10000 events with 662 keV pho<strong>to</strong>ns<br />

were simulated and the amount of produced pho<strong>to</strong> electrons was only<br />

recorded if the incident pho<strong>to</strong>n was completely absorbed. This was<br />

the case <strong>for</strong> about 5900 events. The mean values of the recorded pho<strong>to</strong><br />

electron number and the relative standard deviation <strong>for</strong> the different<br />

readout areas and quantum efficiencies are listed in table 5.5.<br />

RESULTS<br />

The crucial point of this simulation is the limited knowledge about the<br />

actual optical properties of individual crystals. This simulation can<br />

there<strong>for</strong>e give only an estimation of the expected numbers of detected<br />

pho<strong>to</strong> electrons. Properties, like the optical absorption length, depend<br />

on the crystal quality and production process. The increase of the optical<br />

absorption length from 10 cm <strong>to</strong> 100 cm, improves the simulated<br />

amount of detected pho<strong>to</strong>ns significantly by almost a fac<strong>to</strong>r of 10. This<br />

simulation is nevertheless useful <strong>for</strong> comparing the spectral matching<br />

and the influence of the size of different readout devices.

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