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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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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.

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