Development of a Liquid Scintillator and of Data ... - Borexino - Infn
Development of a Liquid Scintillator and of Data ... - Borexino - Infn
Development of a Liquid Scintillator and of Data ... - Borexino - Infn
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4 Position Reconstruction <strong>of</strong> Scintillation Events<br />
scintillator volume, but deposit a fraction <strong>of</strong> their energy in the scintillator. Monte Carlo simulations<br />
<strong>of</strong> these background events yield their ‘center <strong>of</strong> light’ position, which then has to be<br />
folded with the estimated energy resolution to give a meaningful prediction.<br />
For BOREXINO the behaviour is very similar to the CTF (see fig. 4.10). The position resolution<br />
for the pointlike beta events is a little bit better than in the CTF, due to the higher photoelectron<br />
yield ( pe/MeV for BOREXINO, pe/MeV for the CTF). The larger detector<br />
size however gives rise to a bigger time spread due to scattering <strong>and</strong> absorption/reemission<br />
processes. The energy dependence <strong>of</strong> the spatial resolution is<br />
60<br />
Ü<br />
Ô ÒÔ<br />
Ñ<br />
Ñ<br />
Ô ÅÎ <br />
Figure 4.10: Energy dependence <strong>of</strong> the position resolution for beta <strong>and</strong> gamma events starting<br />
from the center <strong>of</strong> the BOREXINO Inner Vessel.