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

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

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

Figure 5.31: Corre<strong>la</strong>ted background spectrum obtained by combing FN and<br />

SM spectra. The linear fit provi<strong>de</strong>s a positive slope of (1.3 ± 1.4)/(3 MeV) 2<br />

and a<br />

2 /dof =4.9/8. The total corre<strong>la</strong>ted background rate is found to be<br />

(0.93 ± 0.26) cpd.<br />

tion of the high energy spectral shape to the low energy intro<strong>du</strong>ce a bias.<br />

With the analysis <strong>de</strong>veloped in this chapter, the obtained pure sample of<br />

corre<strong>la</strong>ted background allow to infer directly the FN and the SM spectral<br />

shape at low energy, without any assumption.<br />

An in<strong>de</strong>pen<strong>de</strong>nt analysis has been performed taking advantage from the<br />

muon tagging capability of the OV in Sec. 5.3. The tagged spectra for<br />

both FN and SM are well <strong>de</strong>scribed by a linear mo<strong>de</strong>l. The linear fit to<br />

the FN spectra provi<strong>de</strong>s a positive slope of (0.17 ± 0.08)/(3 MeV) 2 with<br />

2 /dof = 12.6/8, while the linear fit to the SM spectra provi<strong>de</strong>s a negative<br />

slope of ( 0.14 ± 0.14)/(3 MeV) 2 with 2 /dof = 11.3/8. Background<br />

rates of (0.44 ± 0.14) cpd and (0.48 ± 0.11) cpd are found for FN and SM<br />

respectively. The OVT results are found in agreement with the in<strong>de</strong>pen<strong>de</strong>nt<br />

results obtained from the IVT and the SM analysis <strong>de</strong>veloped in this<br />

chapter. The background rates obtained so far with three di↵erent analysis,<br />

performed without the OVV, are summarised in Tab. 5.17.

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