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

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5.2 High energy analysis 113<br />

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

s)<br />

Entries/(2 "<br />

10 -1<br />

10 -2<br />

-3<br />

10<br />

Entries 434<br />

2<br />

/ ndf<br />

45.03 / 38<br />

Prob 0.2012<br />

c SM<br />

2.229 !<br />

0.273<br />

c FN<br />

1.039 !<br />

0.094<br />

SM<br />

2.178 !<br />

0.317<br />

31.15 !<br />

4.85<br />

0 10 20 30 40 50 60 70 80 90 100<br />

FN<br />

Time (" s)<br />

Figure 5.3: Time corre<strong>la</strong>tion b<strong>et</strong>ween prompt and <strong>de</strong><strong>la</strong>yed events with<br />

prompt in [12, 30] MeV. The histogram is fitted by a two exponential mo<strong>de</strong>l<br />

in or<strong>de</strong>r to <strong>de</strong>scribe the short time corre<strong>la</strong>tion, ⌧ ⇠ 2.2 µs, <strong>du</strong>e to SM (blue<br />

dashed line) and the longer time corre<strong>la</strong>tion, ⌧ ⇠ 30 µs, <strong>du</strong>e to FN (red<br />

dashed line). FN and SM components are separated by imposing a cut on<br />

the time corre<strong>la</strong>tion. The cut e ciency and purity for each component are<br />

estimated using the exponential mo<strong>de</strong>l.

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