Objectives of the Shashlyk Calorimeter
- π/e discrimination
- energy, position and time measurement
TPR Layout of a Shashlyk module
Number of layers | 378 |
Scintillator layer thickness | 1.5 mm |
Lead layer thickness | 0.275 mm |
Effective Moliere radius | 59.8 mm |
Radiation depth | 20 X0 |
Lateral dimensions | 110 x 110 mm2 |
|
Energy resolution | 4.% / sqrt(E) |
Time resolution | 100 ps / sqrt(E) |
Results of simulations
Piotr Hawranek performed simulations of the calorimeter electron/pion separation (Panda meeting Dec'06). He used the so-called
old code.
Simulation comprised:
- π- and e- beams of 1 and 5 GeV/c momentum
- setup with modules of various lateral dimensions
Detector response and cuts imposed in order to select electrons of 5
GeV/c momentum in the 110 x 110 mm
2 modules are shown as an example of the procedure.
Results of the simulations are summarised in the table below.
Module size | e- identified | π- identified as e- |
30 x 30 mm2 | 84.6% | 0.2% |
55 x 55 mm2 | 93.3% | 0.4% |
110 x 110 mm2 | 97.4% | 0.8% |
Module size | e- identified | π- identified as e- |
55 x 55 mm2 | 96.2% | 4.7% |
110 x 110 mm2 | 98.1% | 8.7% |
It should be stressed here, that the analysis procedure was rather rough. Certainly, application of a more sophisticated tools (
e.g. Bayes theorem) could improve the results. The trend, however, is clear already from the presented numbers.
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AleksandraWronska - 26 Apr 2006