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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 />

pressed in U <strong>and</strong> Th equivalents [Ali98c]:<br />

<br />

<br />

ÈÓ<br />

Í ¦ ¢ <br />

ÈÓ Ì ¦ ¢ <br />

There were, however, strong indications that the observed Po coincidence rate was<br />

not due to the scintillator intrinsic radioactivity, but rather due to the diffusion <strong>of</strong> Rn from<br />

the shielding water through the nylon vessel into the scintillator, as the coincidence rate increased<br />

with the Rn level in the shielding water.<br />

By studying the radial distribution <strong>of</strong> all the background events, they could be divided into<br />

an internal <strong>and</strong> external contribution. The total internal background with energies in the neutrino<br />

window (250 - 800 keV) went down from ( ¦ ) counts/day before purification to<br />

( ¦ ) counts/day after the purification operations (nitrogen sparging, water extraction, distillation)<br />

[Ali98c].<br />

40<br />

Figure 3.3: Low energy spectrum measured in the CTF, with the fit <strong>of</strong>a C beta spectrum.<br />

Taken from [Ali98b].

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