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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6 Test <strong>of</strong> a PXE based scintillator for <strong>Borexino</strong><br />
Energy Resolution<br />
The energy resolution can be derived from the width <strong>of</strong> the Po alpha peak (see fig. 6.9):<br />
¡<br />
<br />
<br />
<br />
Ideally, the relative energy resolution should be directly proportional to Ô ÒÔ, where ÒÔ is<br />
the number <strong>of</strong> photoelectrons. This leads to<br />
¡<br />
<br />
<br />
Ô ÒÔ<br />
or ¡<br />
Ô Î <br />
The energy resolution can also be obtained by the fit tothe C spectrum, which gives<br />
¡<br />
Ô ¦ Î <br />
<br />
Res01℄<br />
Again, the values obtained in two different energy regions are in good agreement.<br />
Spatial Resolution<br />
The spatial resolution can be derived without introducing a radioactive source using the correlated<br />
decays <strong>of</strong> Bi <strong>and</strong> Po, which due to the short lifetime <strong>of</strong> the Po must occur at<br />
the same place. Plotting the distance between the x-coordinates <strong>of</strong> the reconstructed positions<br />
<strong>of</strong> the Bi <strong>and</strong> the following Po event gives a distribution with a resolution <strong>of</strong> Ü ¡ Ô .<br />
This resolution is averaged over the energy range <strong>of</strong> the Bi ¬ events (0 - 3.2 MeV) <strong>and</strong> the<br />
Po « events (0.7 - 1.2 MeV). The result is shown in fig. 6.10. As the Rn is distributed<br />
homogeneously inside the scintillator, this method gives the position resolution averaged over<br />
the whole scintillator volume. The results are<br />
94<br />
Ü ¦ Ñ<br />
Ý ¦ Ñ<br />
Þ ¦ Ñ