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Track confidence level cut

NA44 tracks particles in the volume behind the magnetic channel. In the MUL1 (see subsection  3.4.3) runs, the predominant majority of events are single track ones, and our tracking situation is the simplest possible in a heavy ion experiment. Which devices are used to track particles, and which information they provide, is described in subsection  3.8.1. The tracks are fitted with straight lines in three dimensions. In the process, one obtains two $ \chi^2$ values (vertical and horizontal), which, for given number of degrees of freedom $ NDF$, characterize the quality of the fit. For given $ \chi^2$ and $ NDF$, we calculate the probability that a random variable from a true $ \chi^2$ distribution with given $ NDF$ happens to be larger than the given $ \chi^2$ value.

Figure 4.8: Track confidence level distribution in the positive strong field, high angle, pion trigger setting. Top: confidence level distribution in $ X$. Bottom: confidence level distribution in $ Y$.
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Examples of such distributions are shown in Fig. 4.8. We call this probability a confidence level, cut on it from below and call that a confidence level cut, or $ CL$-cut. In experimental data (and in a realistic MC), due to a number of instrumental imperfections (detector off-set, fake hits, inefficiencies) and deviations of the real tracks from the idealistic fitting model (decays, conversions, multiple scattering) the percentage of tracks actually rejected by a sufficiently low $ CL$-cut is much higher than what the ``nominal'' value of the confidence level implies.

To get rid of the unreliable tracks in the off-line analysis of the experimental data, I rejected tracks with either vertical or horizontal $ CL < 10\%$. To evaluate the probability for a real track to be lost as a result of that, I ran MC simulation (thus modeling some of the imperfections mentioned above), and found out that the combined 2D $ CL$-cut retains from 83% to 87% of the good tracks, slightly depending on the setting used. The corresponding corrections (known with 4 digit precision) were applied for each setting.


next up previous contents
Next: Pad Chamber in the Up: Track identification Previous: Double beam cut   Contents
Mikhail Kopytine 2001-08-09