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Experiment Proposal - opera - Infn

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confirmation. Each stopping point is classified as follows by checking the existence of other charged<br />

secondary tracks and of a parent track<br />

• Type-1 vertex: a vertex with a charged parent track. This includes charged-charm decays, τ decays<br />

and charged secondary-interactions. All parent tracks are followed up again and their stopping<br />

points are classified;<br />

• Type-2 vertex: a vertex with no parent and two charged-secondaries with small opening angle.<br />

Electron pairs belong to this category;<br />

• Type-3 vertex: a vertex with no parent and not classified as Type-2. ν interactions, neutral charm<br />

decays and neutral secondary interactions are included in this category.<br />

For a large part of the events the most upstream stopping point is classified as Type-3 and it needs to<br />

be confirmed as a ν interaction. Neutral-charm decays and neutral secondary-interactions misidentified as<br />

ν interaction vertices are taken into account in the calculations of the location efficiency (see Section 7.3.3).<br />

In the case that all stopping points are confirmed as Type-2, a special scanning is applied as described<br />

below, in order to reach the ν interaction point. An example of the vertex confirmation in a brick is shown<br />

in Fig. 107 using Net Scan data from DONUT, used to simulate the OPERA experimental conditions.<br />

Afractionofτ → e decays in QE ν τ interactions are expected to have no hadrons from the primary<br />

interaction reaching the SS film, as illustrated in Fig. 108. Only shower electron pairs, initiated by a<br />

τ decay daughter, reach the SS in that event. Following up these tracks, one would end up at their<br />

conversion point and not at the primary vertex. This is a source of inefficiency in the location of that<br />

class of events.<br />

In order to improve the location efficiency for QE τ → e decays a general scan in a 7 × 7 mm 2<br />

area around the stopping points is performed, to pickup parent electrons. These tracks are then followed<br />

up to reach the primary vertex. Another way to increase the efficiency is to perform a general scanning<br />

in the middle film of the brick, in addition to the above method. Although it requires more scanning<br />

time, it could however be applicable for those events for which the primary vertex confirmation failed<br />

(see Section 6.3.1).<br />

6.3.2 ν τ candidate selection<br />

When a vertex is found Net Scan is applied to a larger volume around it in order to detect a possible<br />

decay topology. Most of the τ are expected to decay within 1 mm from the primary ν interaction.The<br />

analysis is focused on the search of a kink decay topology since the multiprong τ decay modes do not<br />

bring a significant improvment of the experiment sensitivity.<br />

The aim of this step is to filter out events with no sign of a possible decay topology and thus<br />

to reduce the number of events to be fully analysed. The selection is mainly based on topological<br />

information. Momentum roughly measured by multiple scattering in the brick is only used to reject kink<br />

like topologies due to low momentum particles. The emulsion area scanned for this purpose is about<br />

5 mm × 5 mm × 10 films.<br />

138

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