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Experiment Proposal - opera - Infn

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Table 25: Expected background from hadron reinteractions. The contribution as a function of the track<br />

multiplicity at the primary vertex is also given. The numbers are normalised to 10 6 DIS events.<br />

Events HM LM Short Total<br />

ν µ NC 2.1 0.6 4.1 6.8<br />

ν µ CC 2.3 ≪ 0.1 2.0 4.3<br />

Total 4.4 0.6 6.1 11.1<br />

Table 26: Expected background for the different channels. The numbers are normalised to 10 6<br />

events.<br />

DIS<br />

τ → e τ → µ τ → h Total Error<br />

Long: charm 7.0 1.4 7.0 15.4 ±15%<br />

Long: ν e CC<br />

and π 0 0.2 - - 0.2 ±10%<br />

Long: µ scatt. - 5.0 - 5.0 ±50%<br />

Long: had. reint. - - 5.0 5.0 ±50%<br />

Long total 7.2 6.4 12.0 25.6 -<br />

Short: charm 1.1 - (1.3) 1.1 ±15%<br />

Short: ν e CC<br />

and π 0 0.1 - - 0.1 ±10%<br />

Short:had.reint. - - (6.1) (6.1)<br />

Short Total 1.2 - - 1.2<br />

Total 8.4 6.4 12.0 26.8<br />

This background has been evaluated by simulating 1 × 10 7 NC and CC events with GEANT 3.21.<br />

The results are shown in Table 25.<br />

Hadron reinteractions can also contribute to the τ → µ channel when a hadron, produced either in<br />

ν µ NC or ν µ CC interactions with the muon not identified, is misidentified as a muon (see Section 7.3.5).<br />

The evaluation of this background is in progress.<br />

Data on hadronic reinteractions are being analysed [88, 89]. An experimental evaluation of the reinteraction<br />

background is expected soon. In the present situation of the analysis and given the large Monte<br />

Carlo uncertainties, we presently assume a 50% error on this background.<br />

7.5 Sensitivity to ν µ ↔ ν τ oscillations<br />

For the evaluation of the sensitivity of the experiment we assumed the τ detection efficiencies given in<br />

Section 7.3.11 and the backgrounds in Table 26, with the referred to uncertainties.<br />

Since we do not plan to replace with new bricks those which are removed for the event analysis, but<br />

rather with peripheral bricks, the mass of the detector decreases as a function of the exposure time. In<br />

192

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