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

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90 4. Measurement of ✓ 13 with the Double Chooz far d<strong>et</strong>ector<br />

number of entries [per 20ms]<br />

45<br />

40<br />

35<br />

30<br />

25<br />

20<br />

15<br />

10<br />

5<br />

0<br />

Entries 16975<br />

2<br />

! / ndf<br />

1173.6 / 988<br />

Li-9 rate 1.2203 ±<br />

0.1287<br />

constant 15.557 ±<br />

0.128<br />

2000 4000 6000 8000 10000 12000 14000 16000 18000 20000<br />

"t [ms]<br />

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

Figure 1: t-fit for the Li-re<strong>du</strong>ced analysis (E µ > 600 MeV). Data points with error bars are<br />

shown in b<strong>la</strong>ck, the fit result as a solid red line.<br />

Figure 4.12: Time corre<strong>la</strong>tion b<strong>et</strong>ween ¯⌫ e -like candidates and suitable parent<br />

muon, for E µ > 600 MeV. The distribution is fit with an exponential<br />

and a f<strong>la</strong>t component. The exponential component allow to estimate the 9 Li<br />

rate pro<strong>du</strong>ced by high energy muon to be (0.95 ± 0.11) cpd<br />

cumu<strong>la</strong>tive number of events [normalized]<br />

1<br />

0.8<br />

0.6<br />

while the rate for events far from the muon track is extrapo<strong>la</strong>ted based on<br />

the <strong>la</strong>teral distance profile<br />

0.4<br />

b<strong>et</strong>ween muon and 9 Li candidate observed for<br />

high energy muons. A0.2rate of 1.08 ± 0.36(stat) ± 0.25(syst) cpd is obtained.<br />

Lithium<br />

Lastly, the 9 Li rate pro<strong>du</strong>ced by low energy muons neutrons (E< 275 MeV, muons<br />

0<br />

0 0.5 1 1.5 2 2.5 3<br />

crossing the bu↵er and fraction of the<strong>la</strong>teral gamma-catcher) distance from muon track [m] is estimated from the<br />

fit of the t distribution and it is found compatible with zero. An upper<br />

Figure 2: LDP of 9 Li and cosmic neutron capture events with respect to parent HE muon tracks<br />

limit of < 0.3<br />

(E µ<br />

cpd is established by the fit of the t distribution for events<br />

> 600 MeV). Data points are obtained by fitting (Li) or counting (n) all events within a<br />

near the muon given distance track cut from (d the < track, 0.8 m). and normalizing to the rate at 5 m (not shown). While there<br />

are some di↵erences visible for short distances (d 600 MeV shower into the d<strong>et</strong>ector, they are<br />

been found as the most likely the parents of 9 Li isotopes. For this reason the<br />

0.5 ms v<strong>et</strong>o is applied to the ¯⌫ e selection, after a showering muon of energy<br />

above 600 MeV. The <strong>de</strong>finition of parent muon and the v<strong>et</strong>o condition were<br />

varied to obtain the maximum v<strong>et</strong>o e ciency for a fixed <strong>de</strong>ad exposures of<br />

⇠5 %.There<strong>du</strong>ced 9 Li background rate is 1.25 ± 0.54 cpd [98].<br />

Fig. 4.13 shows the 9 Li spectrum, obtained by selecting a purer sample of<br />

9 Li events subtracting the ¯⌫ e background through o↵-time selection. The<br />

obtained spectrum is then compared with MC simu<strong>la</strong>tion of the possible 9 Li<br />

<strong>de</strong>cay branches [56]. The<br />

2 test performed b<strong>et</strong>ween data and MC spectra

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