Effect of the drift field on avalanche gain and charge collection in microgap detectors at high pressure

Detalhes bibliográficos
Autor(a) principal: Fraga, F. A. F.
Data de Publicação: 1998
Outros Autores: Marques, R. Ferreira, Gonçalves, J. A. C., Gonçalo, J. R., Policarpo, A. J. P. L, Eijk, C. W. E. van, Hollander, R. W., Berg, F. van den
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos)
Texto Completo: http://hdl.handle.net/10316/4560
https://doi.org/10.1016/S0168-9002(98)00863-8
Resumo: One of the main drawbacks of the use of microgap structures when used at high pressure (6 bar) at high count rates (~106 s-1 mm-2) is the limited maximum safe gain at which they can be operated. The use of a preamplification device such as the GEM (gas electron multiplier) can overcome this limitation; however, secondary space charge effects due to charge accumulation at the non-metallic surfaces cannot be neglected and should be minimised. These positive charges are due to the intrinsic multiplication of the GEM device and also to the drift of ions from the anode of the main detector. In this study we present data on the variation of the positive ion collection by the drift electrode versus drift field at several pressures up to 6 bar using a Kr-CO2 mixture. Data were collected with microgaps having several anode and insulator widths. The influence of the drift field in the pulse rise time is also considered.
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spelling Effect of the drift field on avalanche gain and charge collection in microgap detectors at high pressureOne of the main drawbacks of the use of microgap structures when used at high pressure (6 bar) at high count rates (~106 s-1 mm-2) is the limited maximum safe gain at which they can be operated. The use of a preamplification device such as the GEM (gas electron multiplier) can overcome this limitation; however, secondary space charge effects due to charge accumulation at the non-metallic surfaces cannot be neglected and should be minimised. These positive charges are due to the intrinsic multiplication of the GEM device and also to the drift of ions from the anode of the main detector. In this study we present data on the variation of the positive ion collection by the drift electrode versus drift field at several pressures up to 6 bar using a Kr-CO2 mixture. Data were collected with microgaps having several anode and insulator widths. The influence of the drift field in the pulse rise time is also considered.http://www.sciencedirect.com/science/article/B6TJM-3VHW9D0-1H/1/7e6cb7ab07e3df379a279e38a943af611998info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articleaplication/PDFhttp://hdl.handle.net/10316/4560http://hdl.handle.net/10316/4560https://doi.org/10.1016/S0168-9002(98)00863-8engNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 419:2-3 (1998) 460-463Fraga, F. A. F.Marques, R. FerreiraGonçalves, J. A. C.Gonçalo, J. R.Policarpo, A. J. P. LEijk, C. W. E. vanHollander, R. W.Berg, F. van deninfo:eu-repo/semantics/openAccessreponame:Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos)instname:Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informaçãoinstacron:RCAAP2022-05-25T03:12:33Zoai:estudogeral.uc.pt:10316/4560Portal AgregadorONGhttps://www.rcaap.pt/oai/openaireopendoar:71602024-03-19T20:59:52.007819Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos) - Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informaçãofalse
dc.title.none.fl_str_mv Effect of the drift field on avalanche gain and charge collection in microgap detectors at high pressure
title Effect of the drift field on avalanche gain and charge collection in microgap detectors at high pressure
spellingShingle Effect of the drift field on avalanche gain and charge collection in microgap detectors at high pressure
Fraga, F. A. F.
title_short Effect of the drift field on avalanche gain and charge collection in microgap detectors at high pressure
title_full Effect of the drift field on avalanche gain and charge collection in microgap detectors at high pressure
title_fullStr Effect of the drift field on avalanche gain and charge collection in microgap detectors at high pressure
title_full_unstemmed Effect of the drift field on avalanche gain and charge collection in microgap detectors at high pressure
title_sort Effect of the drift field on avalanche gain and charge collection in microgap detectors at high pressure
author Fraga, F. A. F.
author_facet Fraga, F. A. F.
Marques, R. Ferreira
Gonçalves, J. A. C.
Gonçalo, J. R.
Policarpo, A. J. P. L
Eijk, C. W. E. van
Hollander, R. W.
Berg, F. van den
author_role author
author2 Marques, R. Ferreira
Gonçalves, J. A. C.
Gonçalo, J. R.
Policarpo, A. J. P. L
Eijk, C. W. E. van
Hollander, R. W.
Berg, F. van den
author2_role author
author
author
author
author
author
author
dc.contributor.author.fl_str_mv Fraga, F. A. F.
Marques, R. Ferreira
Gonçalves, J. A. C.
Gonçalo, J. R.
Policarpo, A. J. P. L
Eijk, C. W. E. van
Hollander, R. W.
Berg, F. van den
description One of the main drawbacks of the use of microgap structures when used at high pressure (6 bar) at high count rates (~106 s-1 mm-2) is the limited maximum safe gain at which they can be operated. The use of a preamplification device such as the GEM (gas electron multiplier) can overcome this limitation; however, secondary space charge effects due to charge accumulation at the non-metallic surfaces cannot be neglected and should be minimised. These positive charges are due to the intrinsic multiplication of the GEM device and also to the drift of ions from the anode of the main detector. In this study we present data on the variation of the positive ion collection by the drift electrode versus drift field at several pressures up to 6 bar using a Kr-CO2 mixture. Data were collected with microgaps having several anode and insulator widths. The influence of the drift field in the pulse rise time is also considered.
publishDate 1998
dc.date.none.fl_str_mv 1998
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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status_str publishedVersion
dc.identifier.uri.fl_str_mv http://hdl.handle.net/10316/4560
http://hdl.handle.net/10316/4560
https://doi.org/10.1016/S0168-9002(98)00863-8
url http://hdl.handle.net/10316/4560
https://doi.org/10.1016/S0168-9002(98)00863-8
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. 419:2-3 (1998) 460-463
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eu_rights_str_mv openAccess
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