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(26 Apr 2006,
AleksandraWronska
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---++ Objectives of the Shashlyk Calorimeter * *π/e discrimination* * energy, position and time measurement ---++ TPR Layout of a Shashlyk module <table border="0" cellspacing="0" cellpadding="0"> <tr> <td width="200"> Number of layers </td> <td> 378</td> </tr> <tr> <td> Scintillator layer thickness </td> <td> 1.5 mm </td> </tr> <tr> <td> Lead layer thickness </td> <td> 0.275 mm </td> </tr> <tr> <td> Effective Moliere radius </td> <td> 59.8 mm </td> </tr> <tr> <td> Radiation depth </td> <td> 20 X<sub>0</sub> </td> </tr> <tr> <td> Lateral dimensions </td> <td> 110 x 110 mm<sup>2</sup></td> </tr> <tr> <td collspan="2"> </td> </tr> <tr> <td>Energy resolution </td> <td> 4.% / sqrt(E) </td> </tr> <tr> <td> Time resolution </td> <td> 100 ps / sqrt(E) </td> </tr> </table> ---++ 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<sup>-</sup> and e<sup>-</sup> 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<sup>2</sup> modules are shown as an example of the procedure. <br /> <center> <img src="%ATTACHURLPATH%/ecal.gif" alt="" width="50%" /> </center> Results of the simulations are summarised in the table below. * *5 GeV/c* <table border="1" cellspacing="0" cellpadding="0"> <tr> <td width="120" align="center"><b>Module size</b></td> <td width="120" align="center"><b>e<sup>-</sup> identified</b></td> <td align="center" width="120"><b>π<sup>-</sup> identified as e<sup>-</sup></b></td> </tr> <tr> <td align="center">30 x 30 mm<sup>2</sup></td> <td align="center">84.6%</td> <td align="center">0.2%</td> </tr> <tr> <td align="center">55 x 55 mm<sup>2</sup></td> <td align="center">93.3%</td> <td align="center">0.4%</td> </tr> <tr> <td align="center">110 x 110 mm<sup>2</sup></td> <td align="center">97.4%</td> <td align="center">0.8%</td> </tr> </table> * *1 GeV/c* <table border="1" cellspacing="0" cellpadding="0"> <tr> <td width="120" align="center"><b>Module size</b></td> <td align="center" width="120"><b>e<sup>-</sup> identified</b></td> <td align="center" width="120"><b>π<sup>-</sup> identified as e<sup>-</sup></b></td> </tr> <tr> <td align="center">55 x 55 mm<sup>2</sup></td> <td align="center">96.2%</td> <td align="center">4.7%</td> </tr> <tr> <td align="center">110 x 110 mm<sup>2</sup></td> <td align="center">98.1%</td> <td align="center">8.7%</td> </tr> </table> 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. -- Main.AleksandraWronska - 26 Apr 2006
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26 Apr 2006 - 07:58
AleksandraWronska
pi/e separation
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Topic revision: r1 - 26 Apr 2006,
AleksandraWronska
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