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

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172 LIST OF FIGURES<br />

4.16 Trigger e ciency as function of energy. The trigger e ciency<br />

is of about 50 % at 0.4 MeV and 100.0 0.0<br />

0.1 % at 0.7 MeV<br />

(prompt lower cut). Above 0.8 MeV the trigger e ciency is<br />

100.0 ± 0.0 %. . . . . . . . . . . . . . . . . . . . . . . . . . . . 94<br />

4.17 Trigger e ciency uncertainty breakdown. Uncertainty on the<br />

trigger e ciency comes mainly from statistical fluctuation,<br />

<strong>de</strong>finition of trigger release time, energy conversion and from<br />

the m<strong>et</strong>hod itself. . . . . . . . . . . . . . . . . . . . . . . . . 95<br />

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

4.18 252 Cf neutron energy spectrum for data and MC (left). Spectral<br />

fit function, used to estimate the fraction on neutron captured<br />

on Gd (right). Due to the 252 Cf neutron multiplicity<br />

(3.869 ± 0.078 neutrons per fission [53]), peaks for the simultaneous<br />

captures of two neutrons on Gd and H (⇠ 10 MeV)<br />

and two captures on Gd (⇠ 16 MeV) are also seen. . . . . . . 96<br />

4.19 t cut e ciency (left) and data/MC discrepancy (right) as a<br />

function of the 252 Cf source position along the z-axis. . . . . . 97<br />

4.20 t cut e ciency (left) and data/MC discrepancy (right) as a<br />

function of the 252 Cf source radial position along gui<strong>de</strong> tube. 97<br />

4.21 t cut e ciency extrapo<strong>la</strong>tion from the d<strong>et</strong>ector center to<br />

the edges. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 97<br />

4.22 E cut e ciency (left) and data/MC discrepancy (right) as<br />

a function of the 252 Cf source radial position along z-axis. . . 98<br />

4.23 E cut e ciency (left) and data/MC discrepancy (right) as<br />

a function of the 252 Cf source radial position along gui<strong>de</strong> tube. 98<br />

4.24 Covariance matrixes <strong>du</strong>e to statistical fluctuation and systematic<br />

uncertainties on the reactor simu<strong>la</strong>tions, the d<strong>et</strong>ector<br />

response and background spectral shape. The matrixes are<br />

drown from MC simu<strong>la</strong>tion. . . . . . . . . . . . . . . . . . . . 103<br />

4.25 Measured prompt energy spectrum for each integration periods<br />

(b<strong>la</strong>ck points) superimposed on the expected prompt energy<br />

spectrum, including backgrounds (green region), for the<br />

non-oscil<strong>la</strong>tion hypothesis (blue dotted histogram) and best<br />

fit (red solid histogram) at sin 2 (2✓ 13 )=0.109±0.030(stat.)±<br />

0.025(syst.) at m 2 31 = 2.32 ⇥ 10 3 eV 2 , with 2 /ndf =<br />

42.1/35 [20]. The insert shown the backgrounds in stacked<br />

histograms. The bottom part of the figure shows both the<br />

di↵erence and the ratio b<strong>et</strong>ween data and non-oscil<strong>la</strong>tion hypothesis<br />

(b<strong>la</strong>ck points), and b<strong>et</strong>ween best fit prediction and<br />

non-oscil<strong>la</strong>tion hypothesis (red solid histogram). . . . . . . . . 104

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