Precision measurement of scaled momentum, charge multiplicity and thrust in $\nu_\mu N$ and $\overline\nu_\mu N$ Interactions

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Every time a trigger in the electronic detectors (see later) is compatible with an interaction inside the target and on time with the beam arrival, the brick with the

The tracking eciency was computed in the simulation by comparing the number of reconstructed tracks and generated charged particles.. Applying the same track selection as used in

In this procedure, once the vertex plate is located by the scan-back track, a search is performed in that emulsion plate for all other tracks reconstructed by the fiber trackers..

The study of events from real data in the region of kinematic variables where a signal is expected may introduce biases in the event selection resulting in incorrect

Two approximate likelihood ratios are formed, both built from the mass of the 3 system (\ a 1 " mass), the masses of the + subsystems (\ " mass), the ratio of the energy

Instead of retting proton candidate tracks with the correct energy loss, an em- pirical correction was applied to the reconstructed proton momentum P REC. This correction, which

Table 7: Systematic uncertainties in units of 10 −2 from the following sources: momentum measurement from tracking in the magnetic field (TPC), energy measurement in the ECAL (ECAL),