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Development of a Liquid Scintillator and of Data ... - Borexino - Infn

Development of a Liquid Scintillator and of Data ... - Borexino - Infn

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3 The Counting Test Facility (CTF) <strong>of</strong> <strong>Borexino</strong><br />

Homogeneous Distribution <strong>of</strong> PMTs<br />

The CTF has 100 PMTs to have a photoelectron (pe) yield big enough to measure energies<br />

as low as a few keV, but only 64 electronic channels (due to funding reasons). Therefore, 72<br />

PMTs are fanned together in pairs, <strong>and</strong> only 28 PMTs are single electronic channels. In the<br />

CTF1 the distribution was chosen as shown in fig. 3.4, a <strong>and</strong> b. Having only few electronic<br />

channels at the top <strong>and</strong> bottom ring leads to a spatial resolution that is much worse in the<br />

z-direction than in the x <strong>and</strong> y direction. As could be shown with a Monte-Carlo simulation<br />

(MC), the spatial resolution can be improved by putting single channels on the top <strong>and</strong> bottom<br />

ring, <strong>and</strong> arranging all the PMTs at the equator rings as double channels (see fig. 3.4, c <strong>and</strong><br />

d). Distributing all the PMTs homogeneously over the rings, improves the homogeneity <strong>of</strong> the<br />

42<br />

Figure 3.4: Schematic drawing <strong>of</strong> the distribution <strong>of</strong> the PMTs <strong>and</strong> electronic channels over the<br />

rings <strong>of</strong> the support structure.

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