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Constant Term Evolution with Lead Plate Thickness Fluctuations in EM Module 0

We report on the results of the Monte Carlo simulation of the module 0 electromagnetic barrel calorimeter. The impact of the thickness variations of the lead plates, which enter in the construction of the module 0, on the energy resolution constant term is presented. Using the real lead plates thick...

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Detalles Bibliográficos
Autores principales: Fleuret, F, Laforge, B, Schwemling, P
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:http://cds.cern.ch/record/683933
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author Fleuret, F
Laforge, B
Schwemling, P
author_facet Fleuret, F
Laforge, B
Schwemling, P
author_sort Fleuret, F
collection CERN
description We report on the results of the Monte Carlo simulation of the module 0 electromagnetic barrel calorimeter. The impact of the thickness variations of the lead plates, which enter in the construction of the module 0, on the energy resolution constant term is presented. Using the real lead plates thickness data which have been used to build the module 0 we find, at $\eta=0.3$ and $\eta=1.1$, a constant term $C < 0.3 \$. The contribution to the constant term coming from lead thickness fluctuations is found to be respectively $C = 0.53 \frac{\sigma^{(5)}}{e_{th}}$ and $C = 0.44 \frac{\sigma^{(5)}}{e_{th}}$ at $\eta=0.3$ and $\eta=1.1$, where $\sigma^{(5)}$ is the standard deviation of the mean lead thickness averaged over 5 plates and $e_{th}$ is the nominal thickness of a single lead plate.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1999
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spelling cern-6839332019-09-30T06:29:59Zhttp://cds.cern.ch/record/683933engFleuret, FLaforge, BSchwemling, PConstant Term Evolution with Lead Plate Thickness Fluctuations in EM Module 0Detectors and Experimental TechniquesWe report on the results of the Monte Carlo simulation of the module 0 electromagnetic barrel calorimeter. The impact of the thickness variations of the lead plates, which enter in the construction of the module 0, on the energy resolution constant term is presented. Using the real lead plates thickness data which have been used to build the module 0 we find, at $\eta=0.3$ and $\eta=1.1$, a constant term $C < 0.3 \$. The contribution to the constant term coming from lead thickness fluctuations is found to be respectively $C = 0.53 \frac{\sigma^{(5)}}{e_{th}}$ and $C = 0.44 \frac{\sigma^{(5)}}{e_{th}}$ at $\eta=0.3$ and $\eta=1.1$, where $\sigma^{(5)}$ is the standard deviation of the mean lead thickness averaged over 5 plates and $e_{th}$ is the nominal thickness of a single lead plate.ATL-LARG-2000-002oai:cds.cern.ch:6839331999-09-22
spellingShingle Detectors and Experimental Techniques
Fleuret, F
Laforge, B
Schwemling, P
Constant Term Evolution with Lead Plate Thickness Fluctuations in EM Module 0
title Constant Term Evolution with Lead Plate Thickness Fluctuations in EM Module 0
title_full Constant Term Evolution with Lead Plate Thickness Fluctuations in EM Module 0
title_fullStr Constant Term Evolution with Lead Plate Thickness Fluctuations in EM Module 0
title_full_unstemmed Constant Term Evolution with Lead Plate Thickness Fluctuations in EM Module 0
title_short Constant Term Evolution with Lead Plate Thickness Fluctuations in EM Module 0
title_sort constant term evolution with lead plate thickness fluctuations in em module 0
topic Detectors and Experimental Techniques
url http://cds.cern.ch/record/683933
work_keys_str_mv AT fleuretf constanttermevolutionwithleadplatethicknessfluctuationsinemmodule0
AT laforgeb constanttermevolutionwithleadplatethicknessfluctuationsinemmodule0
AT schwemlingp constanttermevolutionwithleadplatethicknessfluctuationsinemmodule0