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

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

Upon Digital Q max /Q tot cut, such events disappear. The HELN rejection<br />

e ciency (✏ HELN ) is estimated to be of 99.7 % by the fraction of events<br />

rejected by the cut.<br />

Prompt energy<br />

De<strong>la</strong>yed energy<br />

Entries<br />

2<br />

10<br />

On Time coinci<strong>de</strong>nce<br />

On Time coinci<strong>de</strong>nce + HE LN Cut<br />

Entries/250keV<br />

10<br />

10<br />

1<br />

1<br />

0 5 10 15 20 25 30<br />

prompt E (MeV)<br />

20 25 30 35 40 45 50 55 60 65<br />

<strong>de</strong><strong>la</strong>yed E (MeV)<br />

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

PMT prompt number PMT with Qmax the Qmax (Prompt)<br />

Entries<br />

45<br />

40<br />

35<br />

30<br />

25<br />

20<br />

15<br />

10<br />

5<br />

0<br />

0 50 100 150 200 250 300 350 400<br />

PMTwithQmax<br />

PMT number with the Qmax<br />

PMT <strong>de</strong><strong>la</strong>yed number PMT with the Qmax Qmax (De<strong>la</strong>yed)<br />

Entries<br />

40<br />

35<br />

30<br />

25<br />

20<br />

15<br />

10<br />

5<br />

0<br />

0 50 100 150 200 250 300 350 400<br />

PMTwithQmax<br />

PMT number with the Qmax<br />

Figure 5.28: SM selection with (yellow) and without (withe) Digital<br />

Q max /Q tot cut. SM events are expected below the d<strong>et</strong>ector chimney, so<br />

the PMT with Q max is expected at the top of the d<strong>et</strong>ector (PMT number <<br />

50). After the Digital Q max /Q tot cut a re<strong>du</strong>ction of such events is observed<br />

for the prompt event (bottom left), suggesting the rejection of some physics<br />

events. Assuming the events <strong>de</strong>positing the maximum charge on the PMTs<br />

whose number is < 50 are pure SM events, the physics selection e ciency<br />

is estimated to be 61.7 ± 12.1 %.<br />

Fig. 5.28 shows on-time selection with (yellow) and without (withe) Digital<br />

Q max /Q tot cut. SM events are expected below the d<strong>et</strong>ector chimney, so the<br />

PMT with Q max is expected at the top of the d<strong>et</strong>ector (PMT number <<br />

50). After the Digital Q max /Q tot cut a re<strong>du</strong>ction of such events is observed<br />

in Fig. 5.28 (bottom left), suggesting the rejection of some physics events.<br />

Assuming the events <strong>de</strong>positing the maximum charge on the PMTs whose<br />

number is < 50 are pure SM events, the physics selection e ciency is estimated<br />

to be 61.7 ± 12.1 %. The SM spectrum of Fig. 5.28 (top left) is then<br />

fitted with a f<strong>la</strong>t and a sloped linear mo<strong>de</strong>ls. The SM rate is computed in<br />

agreement with Eq. 5.7, correcting for the Digital Q max /Q tot cut e ciency.<br />

Results are shown in Fig. 5.29 and summarised in Tab. 5.15.

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