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

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5.5 Stopping Muon analysis 145<br />

Source stat. s H/L ✏ t ⇢ t total<br />

[%] [%] [%] [%] [%]<br />

Uncertainty 15.1 40 17.2 7.9 46.8<br />

Table 5.13: Break down of statistical and systematic uncertainties.<br />

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

in<strong>du</strong>ced by the scaling factors. The systematic uncertainties are propagated<br />

to the SM spectrum bin by bin.<br />

The linear fit to the tagged spectrum and its 1 uncertainty are shown in<br />

Fig. 5.25. Both f<strong>la</strong>t and sloped linear mo<strong>de</strong>l are tested and the results are<br />

summarised in Tab. 5.14. The f<strong>la</strong>t linear mo<strong>de</strong>l gives a<br />

2 /ndf =7.1/8 and<br />

a fit probability of ⇠ 52 %. Assuming the fitted f<strong>la</strong>t spectrum, a SM rate of<br />

(0.67±0.10) cpd is obtained. The sloped linear mo<strong>de</strong>l gives a 2 /ndf =6.9/7<br />

and a fit probability of ⇠ 44 %. Assuming the fitted sloped spectrum, a SM<br />

rate of (0.62 ± 0.20) cpd is obtained. Both mo<strong>de</strong>ls shown compatible results<br />

however the more generic sloped shape is used as spectral shape for SM<br />

background, since there is no physical reason for a f<strong>la</strong>t SM spectrum.<br />

Fit const. slope 2 /dof R SM (R SM )/R SM<br />

mo<strong>de</strong>l [1/(3 MeV)] [1/(3 MeV) 2 ] [cpd] [%]<br />

F<strong>la</strong>t 55.8 ± 8.9 – 7.1/8 0.67 ± 0.10 16<br />

Slope 48.8 ± 24.0 0.4 ± 1.3 6.9/7 0.62 ± 0.20 32<br />

Table 5.14: Summary of SM spectra param<strong>et</strong>ers and SM background rate<br />

for the f<strong>la</strong>t and the sloped linear mo<strong>de</strong>l.<br />

5.5.3 Validating high energy light noise rejection<br />

As discussed in the previous section, the LN rejection cuts applied for the<br />

¯⌫ e searches are not enough to reject e ciently the HELN a↵ecting the SM<br />

searches. In [44], the so called Digital Q max /Q tot , <strong>de</strong>fined as the Q max divi<strong>de</strong>d<br />

by the number of ID PMT hits, has been proposed as new variable for<br />

HELN re<strong>du</strong>ction. Such cut is consi<strong>de</strong>red and even optimised in this section<br />

to validate the LN re<strong>du</strong>ction m<strong>et</strong>hod <strong>de</strong>scribed in 5.5.1.<br />

Fig. 5.26 shows distributions of Digital Q max /Q tot vs prompt and <strong>de</strong><strong>la</strong>yed<br />

energy for HELN events and SM candidates. De<strong>la</strong>yed events are clearly distributed<br />

above Digital Q max /Q tot of about 40 while prompt events appear

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