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Experiment Proposal - opera - Infn

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The isolation cuts makes use of the fact that hadron tracks are usually embedded in a hadronic shower,<br />

while the muon track tends to be more isolated. For each plane one computes the distance between the<br />

hit belonging to the candidate muon track and the position of the centroid of all the other hits. Excluding<br />

the first 3 planes after the vertex, the average of this distance is taken as the first discriminating variable<br />

between muons and hadrons.<br />

The second variable is the number of planes containing no other hits than the one belonging to the<br />

track. Tracks for which the average distance from the plane centroid is larger than 20 cm or the number<br />

of planes on which they are isolated is higher than 6 are identified as muons (Fig. 131).<br />

Figure 131: Effect of the topological cut on events with the longest track longer than 10 hits but not<br />

reaching the end of the spectrometer for ν µ CC and NC events. The events falling in the box are classified<br />

as NC.<br />

The combination of range and topology cuts on the longest track in the event results in the efficiencies<br />

shown in Table 13. These efficiencies are calculated on unbiased samples of events before the application<br />

of any other analysis cut. In the complete analysis, the muon identification efficiencies are generally<br />

higher, because low energy events are rejected by other cuts.<br />

In order to increase the identification efficiency for low momentum muons one can also use a method<br />

168

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