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Universit`a degli studi Roma Tre Measurement of the KL meson ...

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30 CHAPTER 3. THE <strong>KL</strong>OE DETECTOR<br />

All signals S above are in ADC counts. S 0,i are <strong>the</strong> zero-<strong>of</strong>fsets <strong>of</strong> <strong>the</strong> amplitude<br />

scale. S mip, i is <strong>the</strong> response for a minimum ionizing particle crossing <strong>the</strong> calorimeter<br />

center. Dividing by S mip, i Eq. 3.4 above accounts for PM response, fiber light yield<br />

and electronics gain. kE gives <strong>the</strong> energy scale in MeV, and it is obtained from<br />

showering particles <strong>of</strong> known energy.<br />

In order to obtain a calorimeter response independent <strong>of</strong> <strong>the</strong> position, a correction<br />

factor Ai A,B (z), due to <strong>the</strong> attenuation along <strong>the</strong> fiber length, is applied. The cell<br />

energy, Ei, is taken as <strong>the</strong> mean <strong>of</strong> <strong>the</strong> determinations at both ends:<br />

Ei(MeV) = Ei AAi A + Ei BAi B<br />

. (3.5)<br />

2<br />

The determination <strong>of</strong> <strong>the</strong> absolute energy scale relies instead on <strong>the</strong> use <strong>of</strong> <strong>the</strong><br />

monochromatic source <strong>of</strong> 510 MeV photons: <strong>the</strong> e + e− → γγ sample. This calibration<br />

is routinely done each 200-400 nb−1 <strong>of</strong> integrated luminosity (i.e., approximately<br />

every 1-2 hours during normal data taking). For <strong>the</strong> timing, <strong>the</strong> relative time <strong>of</strong>fsets<br />

<strong>of</strong> each channel, ti0, related to cable lengths and electronic delays and <strong>the</strong> light<br />

velocity in <strong>the</strong> fibers are evaluated every few days with high momentum cosmic<br />

rays selected with DC information. An iterative procedure uses <strong>the</strong> extrapolation<br />

<strong>of</strong> <strong>the</strong> tracks to <strong>the</strong> calorimeter to minimize <strong>the</strong> residuals between <strong>the</strong> expected and<br />

measured times in each cell. A precision <strong>of</strong> few tens <strong>of</strong> picoseconds is obtained for<br />

<strong>the</strong>se <strong>of</strong>fsets.<br />

The clustering procedure associates different hits in <strong>the</strong> calorimeter cells in a<br />

single cluster as due to <strong>the</strong> same particle. Each group collects hit cells which are<br />

close to each o<strong>the</strong>r. Among <strong>the</strong>se, <strong>the</strong> cell with highest energy release is found;<br />

<strong>the</strong>n, <strong>the</strong> nearest hit cells are associated to that highest one, in order to reconstruct<br />

a cluster.<br />

The cluster energy is obtained by adding <strong>the</strong> energy released in <strong>the</strong> nearest cells:<br />

Eclu = <br />

i<br />

Ei, (3.6)<br />

where i is <strong>the</strong> index <strong>of</strong> <strong>the</strong> cell number.<br />

The cluster position is evaluated as <strong>the</strong> energy-weighted average <strong>of</strong> <strong>the</strong> cell coordinates:<br />

Rclu =<br />

<br />

i Ei Ri<br />

<br />

i Ei<br />

, (3.7)<br />

where Ri = (xi, yi, zi), zi is <strong>the</strong> cell coordinate along <strong>the</strong> fiber (see Eq. 3.3), and<br />

xi, yi are <strong>the</strong> nominal positions <strong>of</strong> <strong>the</strong> cell.<br />

Finally, <strong>the</strong> cluster time is obtained in an analogous way:<br />

<br />

i Eiti<br />

Tclu = , (3.8)<br />

i Ei<br />

where ti are evaluated as in Eq. 3.2.<br />

3.2.2 Time, energy and spatial resolution<br />

After <strong>the</strong> description <strong>of</strong> <strong>the</strong> calibration and monitoring procedures, <strong>the</strong> resolution<br />

<strong>of</strong> <strong>the</strong> calorimeter is here summarized.

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