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

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128 5. Corre<strong>la</strong>ted background<br />

Tag thr. evt. d P/D < 1.5 m evt. d P/D > 1.5 m ✏ d [%]<br />

Mult. 2 3 16 84 ± 8<br />

Mult. 4 2 10 84 ± 11<br />

Mult. 6 1 9 90 ± 9<br />

Table 5.4: Expected number of background events and background rejection<br />

e ciency (✏ d ) with prompt/<strong>de</strong><strong>la</strong>yed distance cut, for di↵erent IVT<br />

multiplicity condition. The background rejection e ciency is in<strong>de</strong>pen<strong>de</strong>nt<br />

from the IVT multiplicity condition, suggesting the systematic re<strong>la</strong>ted to<br />

the background rejection is negligible.<br />

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

shown a distance b<strong>et</strong>ween prompt and <strong>de</strong><strong>la</strong>yed bigger than 1.5 m and are<br />

thus rejected by the distance cut. The remaining background amount to 3<br />

events, corresponding to ⇠ 2 % of the IVT sample. The rejection e ciency<br />

(✏ d ) is estimated to be 84 ± 20 %, the rather big statistical uncertainty is<br />

<strong>du</strong>e to the low statistics avai<strong>la</strong>ble by selecting events with only one o↵<br />

time window.<br />

The number of IVT events selected o↵-time and the background rejection<br />

e ciency are summarised in Tab. 5.4, for di↵erent IVT multiplicity condition.<br />

The rejection e ciency is found constant within statistical uncertainty,<br />

suggesting the systematic re<strong>la</strong>ted to background rejection, intro<strong>du</strong>ced by<br />

the choice of the IVT multiplicity, is negligible.<br />

¯⌫ e +IV<br />

/n background<br />

The ¯⌫ e +IV /n background does not present time nor spatial corre<strong>la</strong>tion<br />

b<strong>et</strong>ween prompt and IV energy <strong>de</strong>positions, as summarised in Tab.<br />

5.3. The spatial and the time distributions b<strong>et</strong>ween prompt and IV energy<br />

<strong>de</strong>positions could then be used as discriminants in or<strong>de</strong>r to separate such<br />

background from the IVT FN. The spatial corre<strong>la</strong>tion has not been evaluated<br />

y<strong>et</strong>, since it requires an IV vertex reconstruction algorithm, which<br />

is currently un<strong>de</strong>r <strong>de</strong>velopment. However, the <strong>de</strong>sign of the IV has been<br />

optimised for tagging high energy <strong>de</strong>position from muons and not to d<strong>et</strong>ect<br />

point-like energy <strong>de</strong>position, as the ID. The IV vertex reconstruction algorithm<br />

is then not expected to show good vertex resolution and consequently<br />

an high background discrimination e ciency is not expected. On the other<br />

hand, the pulse start time is avai<strong>la</strong>ble for both ID and IV waveforms. The<br />

time distribution is expected to show b<strong>et</strong>ter discrimination e ciency than<br />

the spatial distribution, since the time is measured with an uncertainty of<br />

the or<strong>de</strong>r of

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