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Etude et impact du bruit de fond corrélé pour la mesure de l'angle ...

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120 5. Corre<strong>la</strong>ted background<br />

tel-00821629, version 1 - 11 May 2013<br />

Figure 5.8: The IV energy spectrum obtained for di↵erent multiplicity condition.<br />

Requiring the PMT multiplicity to be bigger than 2 rejects most of<br />

the low energy events (< 0.25 MeV), likely <strong>du</strong>e to PMT radioactivity, while<br />

allows to tag physics events from very low energy (> 1.00 MeV).<br />

most of the low energy events, < 0.25 MeV, and allows to tag physics events<br />

with energy > 1.00 MeV. Fig. 5.9 show the vertex distribution of the IVT<br />

sample. As expected for FN events, no corre<strong>la</strong>tions are observed for both<br />

prompt and <strong>de</strong><strong>la</strong>yed events. Fig. 5.10 shows there is no corre<strong>la</strong>tion b<strong>et</strong>ween<br />

the ID and the IV energy <strong>de</strong>positions. Since the IVT rely on the high<br />

multiplicity the FNs are created by their parent muon, the tagged FN is a<br />

separated event from the one interacting in the ID.<br />

Num. PMT hit evt. [0.5;30] MeV evt. [12;30] MeV ✏ IV T [%]<br />

0 7447 199<br />

2 156 65 33 ± 5<br />

4 110 50 25 ± 4<br />

6 94 45 23 ± 4<br />

Table 5.2: Number of IVT events and tagging e<br />

PMT multiplicity.<br />

ciency (✏ IV T ), for di↵erent<br />

Tab. 5.2 summarise the number of events passing IVT, b<strong>et</strong>ween [0.5, 30] MeV<br />

and [12, 30] MeV, where a pure sample of FN is obtained. The ratio of events<br />

in [12, 30] MeV b<strong>et</strong>ween the events passing the IVT over the total, give an

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