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Figure A.3: Horizontal scan events weights map as a funcstion of beam (X,Y)coordinates for QGSP-BERT simulations.
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![Figure 1.3: Cat-away view of the ATLAS calorimeter system [10].](profile/J-Masarik/publication/254468800/figure/fig2/AS:641382708441089@1529928962245/Cat-away-view-of-the-ATLAS-calorimeter-system-10_Q320.jpg)
![Figure 1.4: Sketch of a barrel module [10]. Different layers and...](profile/J-Masarik/publication/254468800/figure/fig3/AS:641382708424721@1529928962594/Sketch-of-a-barrel-module-10-Different-layers-and-electrodes-ganging-in-ph-are_Q320.jpg)
![Figure 1.5: Schematic R − φ and r − z views of the HEC module [10].](profile/J-Masarik/publication/254468800/figure/fig4/AS:641382708416512@1529928962809/Schematic-R-ph-and-r-z-views-of-the-HEC-module-10_Q320.jpg)
The presented thesis brings various contributions to the testing and validation of the ATLAS detector calorimeter calibration. Since the ATLAS calorimeter is non-compensating, the sophisticated software calibration of the calorimeter response is needed. One of the ATLAS official calibration methods is the local hadron calibration. This method is ba...
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NA62 is a fixed target experiment located in the north area of CERN. The ambitious aim of the experiment is the measurement of the branching ratio (Br) of the very rare decay within 10% precision using a decay-in-flight technique. The branching ratio of this decay is very well calculated in the standard model as (9.11 ± 0.72) × 10¹¹ and the measure...
