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

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66 3. The Double Chooz experiment<br />

]<br />

-1<br />

Fission rates [s<br />

90<br />

×10<br />

80<br />

70<br />

60<br />

50<br />

40<br />

30<br />

18<br />

235<br />

U<br />

238<br />

U<br />

239<br />

Pu<br />

241<br />

Pu<br />

20<br />

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

10<br />

0<br />

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

Days<br />

Figure 3.18: Fission rates as function of the day since start of data taking,<br />

as obtained by the simu<strong>la</strong>tion of the reactor evolution. The <strong>de</strong>crease of the<br />

U isotopes and the increase of the Pu isotopes reflect the evolution of the<br />

reactor fuel, which burn U isotopes creating Pu isotopes.<br />

Error (%)<br />

3.5<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

Water Density<br />

Control rod<br />

Co<strong>de</strong><br />

Statistical Error<br />

Initial Burnup<br />

Fuel Temperature<br />

0<br />

50 100 150 200 250 300 350<br />

Days<br />

Figure 3.19: Breakdown of simu<strong>la</strong>tion uncertainties on the 235 U fission rate,<br />

as obtained by varying di↵erent input param<strong>et</strong>ers of the simu<strong>la</strong>tion.

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