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

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5.4 Fast Neutrons analysis 125<br />

Corre<strong>la</strong>tion Fast Neutron -events ¯⌫ e +IV /n<br />

Box 1 Box 2 Box 3<br />

ID only time & space 3 7 3<br />

ID - IV time & space 3 3 7<br />

Table 5.3: Space and time corre<strong>la</strong>tion for IVT fast neutron and its backgrounds<br />

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

On the other hand, -events and ¯⌫ e + IV /n events do not present<br />

both kind of corre<strong>la</strong>tions. The -events shown corre<strong>la</strong>tion b<strong>et</strong>ween the ID<br />

prompt-like event and the IV event, because both are generated by the same<br />

particle, but it <strong>la</strong>cks corre<strong>la</strong>tion b<strong>et</strong>ween the prompt-like and the <strong>de</strong><strong>la</strong>yedlike<br />

event in the ID. The ¯⌫ e +IV /n show corre<strong>la</strong>tion b<strong>et</strong>ween prompt and<br />

<strong>de</strong><strong>la</strong>yed events, since they are generated by a true ¯⌫ e , but it <strong>la</strong>cks the corre<strong>la</strong>tion<br />

b<strong>et</strong>ween the ID event and the IV event, since <strong>du</strong>e to an acci<strong>de</strong>ntal<br />

coinci<strong>de</strong>nce.<br />

Such di↵erent corre<strong>la</strong>tions are exploited in the following two sections to<br />

quantify and reject the background contaminating the IVT sample.<br />

background<br />

In Fig. 5.13 the distance b<strong>et</strong>ween prompt and <strong>de</strong><strong>la</strong>yed events for ¯⌫ e candidates<br />

is shown tog<strong>et</strong>her with the expected distribution from ¯⌫ e MC and the<br />

contribution from acci<strong>de</strong>ntal background. The ¯⌫ e candidates are corre<strong>la</strong>ted<br />

up to ⇠ 1.5 m, while above such distance the distribution is dominated by<br />

the acci<strong>de</strong>ntal background. The FNs are expected to have prompt/<strong>de</strong><strong>la</strong>yed<br />

spatial corre<strong>la</strong>tion simi<strong>la</strong>r to the ¯⌫ e events, while background are expected<br />

to have the same distribution as the acci<strong>de</strong>ntal background.<br />

A comparison b<strong>et</strong>ween the IVT sample and the contamination from<br />

background is shown in Fig 5.14. The sample is obtained by performing<br />

o↵-time window coinci<strong>de</strong>nce b<strong>et</strong>ween [1010, 1100] µs. A total of 19 events<br />

are found, corresponding to ⇠ 12 % of the IVT sample. The background<br />

contaminates, as expected, the low energy part of the energy spectrum, up<br />

to ⇠ 2 MeV on the ID and up to ⇠ 1 MeV on the IV. The FN sample shows<br />

spatial corre<strong>la</strong>tion up to ⇠ 1mwhile background extends beyond 1 m.<br />

The vertex distribution from background shows a distribution close to<br />

the outer most region of the ID, as expected from originating from outsi<strong>de</strong><br />

the ID.<br />

A cut on the distance b<strong>et</strong>ween prompt and <strong>de</strong><strong>la</strong>yed candidate is applied to re<strong>du</strong>ce<br />

background contamination to the IV Tagged sample. The cut value<br />

is s<strong>et</strong> at 1.5 m, where the acci<strong>de</strong>ntal component become dominant, as shown<br />

in Fig. 5.13. Of the 19 events selected with the o↵-time search, 16 events

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