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Inverse Low Gain Avalanche Detectors (iLGADs) for precise tracking and timing applications
Low Gain Avalanche Detector (LGAD) is the baseline sensing technology of the recently proposed Minimum Ionizing Particle (MIP) end-cap timing detectors (MTD) at the Atlas and CMS experiments. The current MTD sensor is designed as a multi-pad matrix detector delivering a poor position resolution, due...
Autores principales: | , , , , , , , , , , , , , , , |
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Formato: | info:eu-repo/semantics/article |
Lenguaje: | eng |
Publicado: |
Nucl. Instrum. Methods Phys. Res., A
2019
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/j.nima.2019.162545 http://cds.cern.ch/record/2673324 |
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author | Currás, E. Carulla, M. Centis Vignali, M. Duarte-Campderros, J. Fernández, M. Flores, D. García, A. Gómez, G. González, J. Hidalgo, S. Jaramillo, R. Merlos, A. Moll, M. Pellegrini, G. Quirion, D. Vila, Iván |
author_facet | Currás, E. Carulla, M. Centis Vignali, M. Duarte-Campderros, J. Fernández, M. Flores, D. García, A. Gómez, G. González, J. Hidalgo, S. Jaramillo, R. Merlos, A. Moll, M. Pellegrini, G. Quirion, D. Vila, Iván |
author_sort | Currás, E. |
collection | CERN |
description | Low Gain Avalanche Detector (LGAD) is the baseline sensing technology of the recently proposed Minimum Ionizing Particle (MIP) end-cap timing detectors (MTD) at the Atlas and CMS experiments. The current MTD sensor is designed as a multi-pad matrix detector delivering a poor position resolution, due to the relatively large pad area, around 1 mm$^2$ ; and a good timing resolution, around 20–30 ps. Besides, in his current technological incarnation, the timing resolution of the MTD LGAD sensors is severely degraded once the MIP particle hits the inter-pad region since the signal amplification is missing for this region. This limitation is named as the LGAD fill-factor problem. To overcome the fill factor problem and the poor position resolution of the MTD LGAD sensors, a p-in-p LGAD (iLGAD) was introduced. Contrary to the conventional LGAD, the iLGAD has a non-segmented deep p-well (the multiplication layer). Therefore, iLGADs should ideally present a constant gain value over all the sensitive region of the device without gain drops between the signal collecting electrodes; in other words, iLGADs should have a 100 % fill-factor by design. In this paper, tracking and timing performance of the first iLGAD prototypes is presented. |
format | info:eu-repo/semantics/article |
id | cern-2673324 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2019 |
publisher | Nucl. Instrum. Methods Phys. Res., A |
record_format | invenio |
spelling | cern-26733242023-03-14T19:24:16Z doi:10.1016/j.nima.2019.162545 http://cds.cern.ch/record/2673324 eng Currás, E. Carulla, M. Centis Vignali, M. Duarte-Campderros, J. Fernández, M. Flores, D. García, A. Gómez, G. González, J. Hidalgo, S. Jaramillo, R. Merlos, A. Moll, M. Pellegrini, G. Quirion, D. Vila, Iván Inverse Low Gain Avalanche Detectors (iLGADs) for precise tracking and timing applications physics.ins-det Detectors and Experimental Techniques 7: Advanced hybrid pixel detectors Low Gain Avalanche Detector (LGAD) is the baseline sensing technology of the recently proposed Minimum Ionizing Particle (MIP) end-cap timing detectors (MTD) at the Atlas and CMS experiments. The current MTD sensor is designed as a multi-pad matrix detector delivering a poor position resolution, due to the relatively large pad area, around 1 mm$^2$ ; and a good timing resolution, around 20–30 ps. Besides, in his current technological incarnation, the timing resolution of the MTD LGAD sensors is severely degraded once the MIP particle hits the inter-pad region since the signal amplification is missing for this region. This limitation is named as the LGAD fill-factor problem. To overcome the fill factor problem and the poor position resolution of the MTD LGAD sensors, a p-in-p LGAD (iLGAD) was introduced. Contrary to the conventional LGAD, the iLGAD has a non-segmented deep p-well (the multiplication layer). Therefore, iLGADs should ideally present a constant gain value over all the sensitive region of the device without gain drops between the signal collecting electrodes; in other words, iLGADs should have a 100 % fill-factor by design. In this paper, tracking and timing performance of the first iLGAD prototypes is presented. Low Gain Avalanche Detector (LGAD) is the baseline sensing technology of the recently proposed Minimum Ionizing Particle (MIP) end-cap timing detectors (MTD) at the Atlas and CMS experiments. The current MTD sensor is designed as a multi-pad matrix detector delivering a poor position resolution, due to the relatively large pad area, around 1 mm 2 ; and a good timing resolution, around 20–30 ps. Besides, in his current technological incarnation, the timing resolution of the MTD LGAD sensors is severely degraded once the MIP particle hits the inter-pad region since the signal amplification is missing for this region. This limitation is named as the LGAD fill-factor problem. To overcome the fill factor problem and the poor position resolution of the MTD LGAD sensors, a p-in-p LGAD (iLGAD) was introduced. Contrary to the conventional LGAD, the iLGAD has a non-segmented deep p-well (the multiplication layer). Therefore, iLGADs should ideally present a constant gain value over all the sensitive region of the device without gain drops between the signal collecting electrodes; in other words, iLGADs should have a 100 % fill-factor by design. In this paper, tracking and timing performance of the first iLGAD prototypes is presented. Low Gain Avalanche Detector (LGAD) is the baseline sensing technology of the recently proposed Minimum Ionizing Particle (MIP) end-cap timing detectors (MTD) at the Atlas and CMS experiments. The current MTD sensor is designed as a multi-pad matrix detector delivering a poor position resolution, due to the relatively large pad area, around 1 $mm^2$; and a good timing resolution, around 20-30 ps. Besides, in his current technological incarnation, the timing resolution of the MTD LGAD sensors is severely degraded once the MIP particle hits the inter-pad region since the signal amplification is missing for this region. This limitation is named as the LGAD fill-factor problem. To overcome the fill factor problem and the poor position resolution of the MTD LGAD sensors, a p-in-p LGAD (iLGAD) was introduced. Contrary to the conventional LGAD, the iLGAD has a non-segmented deep p-well (the multiplication layer). Therefore, iLGADs should ideally present a constant gain value over all the sensitive region of the device without gain drops between the signal collecting electrodes; in other words, iLGADs should have a 100${\%}$ fill-factor by design. In this paper, tracking and timing performance of the first iLGAD prototypes is presented. info:eu-repo/grantAgreement/EC/FP7/654168 info:eu-repo/semantics/openAccess Education Level info:eu-repo/semantics/article http://cds.cern.ch/record/2673324 Nucl. Instrum. Methods Phys. Res., A Nucl. Instrum. Methods Phys. Res., A, (2020) pp. 162545 2019-04-03 |
spellingShingle | physics.ins-det Detectors and Experimental Techniques 7: Advanced hybrid pixel detectors Currás, E. Carulla, M. Centis Vignali, M. Duarte-Campderros, J. Fernández, M. Flores, D. García, A. Gómez, G. González, J. Hidalgo, S. Jaramillo, R. Merlos, A. Moll, M. Pellegrini, G. Quirion, D. Vila, Iván Inverse Low Gain Avalanche Detectors (iLGADs) for precise tracking and timing applications |
title | Inverse Low Gain Avalanche Detectors (iLGADs) for precise tracking and timing applications |
title_full | Inverse Low Gain Avalanche Detectors (iLGADs) for precise tracking and timing applications |
title_fullStr | Inverse Low Gain Avalanche Detectors (iLGADs) for precise tracking and timing applications |
title_full_unstemmed | Inverse Low Gain Avalanche Detectors (iLGADs) for precise tracking and timing applications |
title_short | Inverse Low Gain Avalanche Detectors (iLGADs) for precise tracking and timing applications |
title_sort | inverse low gain avalanche detectors (ilgads) for precise tracking and timing applications |
topic | physics.ins-det Detectors and Experimental Techniques 7: Advanced hybrid pixel detectors |
url | https://dx.doi.org/10.1016/j.nima.2019.162545 http://cds.cern.ch/record/2673324 http://cds.cern.ch/record/2673324 |
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