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Performance characteristics of a gas proportional scintillation counter coupled to a microstrip gas chamber photosensor

Detalhes bibliográficos
Autor(a) principal: Veloso, J. F. C. A.
Data de Publicação: 1999
Outros Autores: Santos, J. M. F. dos, Conde, C. A. N.
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositórios Científicos de Acesso Aberto de Portugal (RCAAP)
Texto Completo: https://hdl.handle.net/10316/4552
Resumo: A P10-filled microstrip gas chamber (MSGC) is used to replace the conventional photomultiplier tube (PMT) as the photosensor for a Gas Proportional Scintillation Counter (GPSC). The Vacuum Ultra-Violet (VUV) scintillation light produced in the xenon-filled GPSC is transmitted through a 1 mm thick high-purity quartz window to the MSGC where it is converted to photoelectrons by a CsI photocathode deposited directly onto the surface of a microstrip plate (MSP). These photoelectrons are afterwards multiplied near the microstrip plate anodes with a charge gain of about 103. The energy resolution achieved for 5.9 keV X-rays is 11.5% which, while not yet as good as the 8% figure for standard GPSC (instrumented with a PMT), is already better than the energy resolution obtained for standard proportional counters. Experimental results are presented and discussed. With this design a compact GPSC is obtained which has the further advantage of being much less sensitive to magnetic fields than PMT-based GPSCs.
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spelling Performance characteristics of a gas proportional scintillation counter coupled to a microstrip gas chamber photosensorGas proportional scintillation counterMicrostrip gas chamber photosensorA P10-filled microstrip gas chamber (MSGC) is used to replace the conventional photomultiplier tube (PMT) as the photosensor for a Gas Proportional Scintillation Counter (GPSC). The Vacuum Ultra-Violet (VUV) scintillation light produced in the xenon-filled GPSC is transmitted through a 1 mm thick high-purity quartz window to the MSGC where it is converted to photoelectrons by a CsI photocathode deposited directly onto the surface of a microstrip plate (MSP). These photoelectrons are afterwards multiplied near the microstrip plate anodes with a charge gain of about 103. The energy resolution achieved for 5.9 keV X-rays is 11.5% which, while not yet as good as the 8% figure for standard GPSC (instrumented with a PMT), is already better than the energy resolution obtained for standard proportional counters. Experimental results are presented and discussed. With this design a compact GPSC is obtained which has the further advantage of being much less sensitive to magnetic fields than PMT-based GPSCs.http://www.sciencedirect.com/science/article/B6TJM-3VR1CVW-1Y/1/d58104484bd3814021599b6308e11a801999info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articleaplication/PDFhttps://hdl.handle.net/10316/4552https://hdl.handle.net/10316/4552engNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 422:1-3 (1999) 273-277Veloso, J. F. C. A.Santos, J. M. F. dosConde, C. A. N.info:eu-repo/semantics/openAccessreponame:Repositórios Científicos de Acesso Aberto de Portugal (RCAAP)instname:FCCN, serviços digitais da FCT – Fundação para a Ciência e a Tecnologiainstacron:RCAAP2021-10-22T11:35:54Zoai:estudogeral.uc.pt:10316/4552Portal AgregadorONGhttps://www.rcaap.pt/oai/openaireinfo@rcaap.ptopendoar:https://opendoar.ac.uk/repository/71602025-05-29T05:21:43.432024Repositórios Científicos de Acesso Aberto de Portugal (RCAAP) - FCCN, serviços digitais da FCT – Fundação para a Ciência e a Tecnologiafalse
dc.title.none.fl_str_mv Performance characteristics of a gas proportional scintillation counter coupled to a microstrip gas chamber photosensor
title Performance characteristics of a gas proportional scintillation counter coupled to a microstrip gas chamber photosensor
spellingShingle Performance characteristics of a gas proportional scintillation counter coupled to a microstrip gas chamber photosensor
Veloso, J. F. C. A.
Gas proportional scintillation counter
Microstrip gas chamber photosensor
title_short Performance characteristics of a gas proportional scintillation counter coupled to a microstrip gas chamber photosensor
title_full Performance characteristics of a gas proportional scintillation counter coupled to a microstrip gas chamber photosensor
title_fullStr Performance characteristics of a gas proportional scintillation counter coupled to a microstrip gas chamber photosensor
title_full_unstemmed Performance characteristics of a gas proportional scintillation counter coupled to a microstrip gas chamber photosensor
title_sort Performance characteristics of a gas proportional scintillation counter coupled to a microstrip gas chamber photosensor
author Veloso, J. F. C. A.
author_facet Veloso, J. F. C. A.
Santos, J. M. F. dos
Conde, C. A. N.
author_role author
author2 Santos, J. M. F. dos
Conde, C. A. N.
author2_role author
author
dc.contributor.author.fl_str_mv Veloso, J. F. C. A.
Santos, J. M. F. dos
Conde, C. A. N.
dc.subject.por.fl_str_mv Gas proportional scintillation counter
Microstrip gas chamber photosensor
topic Gas proportional scintillation counter
Microstrip gas chamber photosensor
description A P10-filled microstrip gas chamber (MSGC) is used to replace the conventional photomultiplier tube (PMT) as the photosensor for a Gas Proportional Scintillation Counter (GPSC). The Vacuum Ultra-Violet (VUV) scintillation light produced in the xenon-filled GPSC is transmitted through a 1 mm thick high-purity quartz window to the MSGC where it is converted to photoelectrons by a CsI photocathode deposited directly onto the surface of a microstrip plate (MSP). These photoelectrons are afterwards multiplied near the microstrip plate anodes with a charge gain of about 103. The energy resolution achieved for 5.9 keV X-rays is 11.5% which, while not yet as good as the 8% figure for standard GPSC (instrumented with a PMT), is already better than the energy resolution obtained for standard proportional counters. Experimental results are presented and discussed. With this design a compact GPSC is obtained which has the further advantage of being much less sensitive to magnetic fields than PMT-based GPSCs.
publishDate 1999
dc.date.none.fl_str_mv 1999
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
dc.type.driver.fl_str_mv info:eu-repo/semantics/article
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dc.identifier.uri.fl_str_mv https://hdl.handle.net/10316/4552
https://hdl.handle.net/10316/4552
url https://hdl.handle.net/10316/4552
dc.language.iso.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 422:1-3 (1999) 273-277
dc.rights.driver.fl_str_mv info:eu-repo/semantics/openAccess
eu_rights_str_mv openAccess
dc.format.none.fl_str_mv aplication/PDF
dc.source.none.fl_str_mv reponame:Repositórios Científicos de Acesso Aberto de Portugal (RCAAP)
instname:FCCN, serviços digitais da FCT – Fundação para a Ciência e a Tecnologia
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collection Repositórios Científicos de Acesso Aberto de Portugal (RCAAP)
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