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Simulation of RPC performance for 511 keV photon detection

Measurements of the time resolution of timing Resistive Plate Chambers (RPCs) reveal some differences when comparing the results for 511 keV photons and for particle beams. The subject is of interest, since timing RPCs are currently considered for Positron Emission Tomography (PET), where the sensit...

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Detalles Bibliográficos
Autores principales: Lippmann, C, Vincke, H, Riegler, W
Lenguaje:eng
Publicado: 2009
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nima.2008.12.102
http://cds.cern.ch/record/1275090
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author Lippmann, C
Vincke, H
Riegler, W
author_facet Lippmann, C
Vincke, H
Riegler, W
author_sort Lippmann, C
collection CERN
description Measurements of the time resolution of timing Resistive Plate Chambers (RPCs) reveal some differences when comparing the results for 511 keV photons and for particle beams. The subject is of interest, since timing RPCs are currently considered for Positron Emission Tomography (PET), where the sensitivity of the system depends largely on the time resolution of the detector. In this publication we discuss possible explanations, in particular the statistical fluctuations of the deposited charge and the Compton electron flight time distributions. Moreover, we rediscuss the reduction of the Townsend coefficient due to the space charge effect inside the avalanches as a function of the avalanche size. We shall see that the dependence assumed by different analytic models differs significantly from what is predicted by detailed Monte Carlo avalanche simulations.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2009
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spelling cern-12750902019-09-30T06:29:59Zdoi:10.1016/j.nima.2008.12.102http://cds.cern.ch/record/1275090engLippmann, CVincke, HRiegler, WSimulation of RPC performance for 511 keV photon detectionDetectors and Experimental TechniquesMeasurements of the time resolution of timing Resistive Plate Chambers (RPCs) reveal some differences when comparing the results for 511 keV photons and for particle beams. The subject is of interest, since timing RPCs are currently considered for Positron Emission Tomography (PET), where the sensitivity of the system depends largely on the time resolution of the detector. In this publication we discuss possible explanations, in particular the statistical fluctuations of the deposited charge and the Compton electron flight time distributions. Moreover, we rediscuss the reduction of the Townsend coefficient due to the space charge effect inside the avalanches as a function of the avalanche size. We shall see that the dependence assumed by different analytic models differs significantly from what is predicted by detailed Monte Carlo avalanche simulations.oai:cds.cern.ch:12750902009
spellingShingle Detectors and Experimental Techniques
Lippmann, C
Vincke, H
Riegler, W
Simulation of RPC performance for 511 keV photon detection
title Simulation of RPC performance for 511 keV photon detection
title_full Simulation of RPC performance for 511 keV photon detection
title_fullStr Simulation of RPC performance for 511 keV photon detection
title_full_unstemmed Simulation of RPC performance for 511 keV photon detection
title_short Simulation of RPC performance for 511 keV photon detection
title_sort simulation of rpc performance for 511 kev photon detection
topic Detectors and Experimental Techniques
url https://dx.doi.org/10.1016/j.nima.2008.12.102
http://cds.cern.ch/record/1275090
work_keys_str_mv AT lippmannc simulationofrpcperformancefor511kevphotondetection
AT vinckeh simulationofrpcperformancefor511kevphotondetection
AT rieglerw simulationofrpcperformancefor511kevphotondetection