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Time response functions and avalanche fluctuations in resistive plate chambers

The time response function of RPCs is derived. First, primary electron distributions in the RPC gas gap are discussed. Then the exact expression for the fluctuations of an avalanche starting with a fixed number of primary electrons is derived, using Legler's model of avalanche multiplication in...

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Detalles Bibliográficos
Autor principal: Riegler, W
Lenguaje:eng
Publicado: 2009
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nima.2008.12.207
http://cds.cern.ch/record/1275092
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author Riegler, W
author_facet Riegler, W
author_sort Riegler, W
collection CERN
description The time response function of RPCs is derived. First, primary electron distributions in the RPC gas gap are discussed. Then the exact expression for the fluctuations of an avalanche starting with a fixed number of primary electrons is derived, using Legler's model of avalanche multiplication in electronegative gases. By means of the Z-Transform formalism, the primary electron distributions and avalanche fluctuations are then combined and an analytic expression for the RPC time response function is derived. The solution is further used to discuss signal threshold and attachment effects. Finally, the time response function is evaluated for several primary ionization models.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2009
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spelling cern-12750922019-09-30T06:29:59Zdoi:10.1016/j.nima.2008.12.207http://cds.cern.ch/record/1275092engRiegler, WTime response functions and avalanche fluctuations in resistive plate chambersDetectors and Experimental TechniquesThe time response function of RPCs is derived. First, primary electron distributions in the RPC gas gap are discussed. Then the exact expression for the fluctuations of an avalanche starting with a fixed number of primary electrons is derived, using Legler's model of avalanche multiplication in electronegative gases. By means of the Z-Transform formalism, the primary electron distributions and avalanche fluctuations are then combined and an analytic expression for the RPC time response function is derived. The solution is further used to discuss signal threshold and attachment effects. Finally, the time response function is evaluated for several primary ionization models.oai:cds.cern.ch:12750922009
spellingShingle Detectors and Experimental Techniques
Riegler, W
Time response functions and avalanche fluctuations in resistive plate chambers
title Time response functions and avalanche fluctuations in resistive plate chambers
title_full Time response functions and avalanche fluctuations in resistive plate chambers
title_fullStr Time response functions and avalanche fluctuations in resistive plate chambers
title_full_unstemmed Time response functions and avalanche fluctuations in resistive plate chambers
title_short Time response functions and avalanche fluctuations in resistive plate chambers
title_sort time response functions and avalanche fluctuations in resistive plate chambers
topic Detectors and Experimental Techniques
url https://dx.doi.org/10.1016/j.nima.2008.12.207
http://cds.cern.ch/record/1275092
work_keys_str_mv AT rieglerw timeresponsefunctionsandavalanchefluctuationsinresistiveplatechambers