Cargando…

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...

Descripción completa

Detalles Bibliográficos
Autores principales: 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
Formato: info:eu-repo/semantics/article
Lenguaje:eng
Publicado: Nucl. Instrum. Methods Phys. Res., A 2019
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nima.2019.162545
http://cds.cern.ch/record/2673324
_version_ 1780962493633396736
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
work_keys_str_mv AT currase inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT carullam inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT centisvignalim inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT duartecampderrosj inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT fernandezm inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT floresd inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT garciaa inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT gomezg inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT gonzalezj inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT hidalgos inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT jaramillor inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT merlosa inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT mollm inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT pellegrinig inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT quiriond inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications
AT vilaivan inverselowgainavalanchedetectorsilgadsforprecisetrackingandtimingapplications