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Deep Diffused APDs for Charged Particle Timing Applications: Performance after Neutron Irradiation

Recent interest in pile-up mitigation through fast timing at the HL-LHC has focused attention on technologies that now achieve minimum ionising particle (MIP) time resolution of 30 picoseconds or less. The constraints of technical maturity and radiation tolerance narrowed the options in this rapidly...

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Autores principales: Centis Vignali, M., Gallinaro, M., Harrop, B., Lu, C., McClish, M., Moll, M., Newcomer, F.M., Otero Ugobono, S., White, S.
Lenguaje:eng
Publicado: 2018
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nima.2019.162930
http://cds.cern.ch/record/2653219
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author Centis Vignali, M.
Gallinaro, M.
Harrop, B.
Lu, C.
McClish, M.
Moll, M.
Newcomer, F.M.
Otero Ugobono, S.
White, S.
author_facet Centis Vignali, M.
Gallinaro, M.
Harrop, B.
Lu, C.
McClish, M.
Moll, M.
Newcomer, F.M.
Otero Ugobono, S.
White, S.
author_sort Centis Vignali, M.
collection CERN
description Recent interest in pile-up mitigation through fast timing at the HL-LHC has focused attention on technologies that now achieve minimum ionising particle (MIP) time resolution of 30 picoseconds or less. The constraints of technical maturity and radiation tolerance narrowed the options in this rapidly developing field for the ATLAS and CMS upgrades to low gain avalanche detectors and silicon photomultipliers. In a variety of applications where occupancies and doses are lower, devices with pixel elements of order 1 cm$^2$, nevertheless achieving 30 ps, would be attractive. In this paper, deep diffused Avalanche Photo Diodes (APDs) are examined as candidate timing detectors for HL-LHC applications. Devices with an active area of $8 \times 8$ mm$^2$ are characterised using a pulsed infrared laser and, in some cases, high energy particle beams.The timing performance as well as the uniformity of response are examined. The effects of radiation damage on current, signal amplitude, noise, and timing of the APDs are evaluated using detectors with an active area of $2 \times 2$ mm$^2$. These detectors were irradiated with neutrons up to a a 1-MeV neutrons fluence $\Phi_{eq} = 10^{15}$ cm$^{-2}$. Their timing performance was characterised using a pulsed infrared laser. While a time resolution of $27 \pm 1$ ps was obtained in a beam test using an $8 \times 8$ mm$^2$ sensor, the present study only demonstrates that gain loss can be compensated by increased detector bias up to fluences of $\Phi_{eq} = 6 \cdot 10^{13}$ cm$^{-2}$. So it possibly falls short of the $\Phi_{eq} = 10^{14}$ cm$^{-2}$ requirement for the CMS barrel over the lifetime of the HL-LHC.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2018
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spelling cern-26532192023-03-14T20:32:13Zdoi:10.1016/j.nima.2019.162930http://cds.cern.ch/record/2653219engCentis Vignali, M.Gallinaro, M.Harrop, B.Lu, C.McClish, M.Moll, M.Newcomer, F.M.Otero Ugobono, S.White, S.Deep Diffused APDs for Charged Particle Timing Applications: Performance after Neutron Irradiationhep-exParticle Physics - Experimentphysics.ins-detDetectors and Experimental TechniquesRecent interest in pile-up mitigation through fast timing at the HL-LHC has focused attention on technologies that now achieve minimum ionising particle (MIP) time resolution of 30 picoseconds or less. The constraints of technical maturity and radiation tolerance narrowed the options in this rapidly developing field for the ATLAS and CMS upgrades to low gain avalanche detectors and silicon photomultipliers. In a variety of applications where occupancies and doses are lower, devices with pixel elements of order 1 cm$^2$, nevertheless achieving 30 ps, would be attractive. In this paper, deep diffused Avalanche Photo Diodes (APDs) are examined as candidate timing detectors for HL-LHC applications. Devices with an active area of $8 \times 8$ mm$^2$ are characterised using a pulsed infrared laser and, in some cases, high energy particle beams.The timing performance as well as the uniformity of response are examined. The effects of radiation damage on current, signal amplitude, noise, and timing of the APDs are evaluated using detectors with an active area of $2 \times 2$ mm$^2$. These detectors were irradiated with neutrons up to a a 1-MeV neutrons fluence $\Phi_{eq} = 10^{15}$ cm$^{-2}$. Their timing performance was characterised using a pulsed infrared laser. While a time resolution of $27 \pm 1$ ps was obtained in a beam test using an $8 \times 8$ mm$^2$ sensor, the present study only demonstrates that gain loss can be compensated by increased detector bias up to fluences of $\Phi_{eq} = 6 \cdot 10^{13}$ cm$^{-2}$. So it possibly falls short of the $\Phi_{eq} = 10^{14}$ cm$^{-2}$ requirement for the CMS barrel over the lifetime of the HL-LHC.Recent interest in pile-up mitigation through fast timing at the HL-LHC has focused attention on technologies that now achieve minimum ionising particle (MIP) time resolution of 30 picoseconds or less. The constraints of technical maturity and radiation tolerance narrowed the options in this rapidly developing field for the ATLAS and CMS upgrades to low gain avalanche detectors and silicon photomultipliers. In a variety of applications where occupancies and doses are lower, devices with pixel elements of order 1 cm$^2$, nevertheless achieving 30 ps, would be attractive. In this paper, deep diffused Avalanche Photo Diodes (APDs) are examined as candidate timing detectors for HL-LHC applications. Devices with an active area of $8 \times 8$ mm$^2$ are characterised using a pulsed infrared laser and, in some cases, high energy particle beams.The timing performance as well as the uniformity of response are examined. The effects of radiation damage on current, signal amplitude, noise, and timing of the APDs are evaluated using detectors with an active area of $2 \times 2$ mm$^2$. These detectors were irradiated with neutrons up to a a 1-MeV neutrons fluence $\Phi_{eq} = 10^{15}$ cm$^{-2}$. Their timing performance was characterised using a pulsed infrared laser. While a time resolution of $27 \pm 1$ ps was obtained in a beam test using an $8 \times 8$ mm$^2$ sensor, the present study only demonstrates that gain loss can be compensated by increased detector bias up to fluences of $\Phi_{eq} = 6 \cdot 10^{13}$ cm$^{-2}$. So it possibly falls short of the $\Phi_{eq} = 10^{14}$ cm$^{-2}$ requirement for the CMS barrel over the lifetime of the HL-LHC.arXiv:1812.08433oai:cds.cern.ch:26532192018-12-20
spellingShingle hep-ex
Particle Physics - Experiment
physics.ins-det
Detectors and Experimental Techniques
Centis Vignali, M.
Gallinaro, M.
Harrop, B.
Lu, C.
McClish, M.
Moll, M.
Newcomer, F.M.
Otero Ugobono, S.
White, S.
Deep Diffused APDs for Charged Particle Timing Applications: Performance after Neutron Irradiation
title Deep Diffused APDs for Charged Particle Timing Applications: Performance after Neutron Irradiation
title_full Deep Diffused APDs for Charged Particle Timing Applications: Performance after Neutron Irradiation
title_fullStr Deep Diffused APDs for Charged Particle Timing Applications: Performance after Neutron Irradiation
title_full_unstemmed Deep Diffused APDs for Charged Particle Timing Applications: Performance after Neutron Irradiation
title_short Deep Diffused APDs for Charged Particle Timing Applications: Performance after Neutron Irradiation
title_sort deep diffused apds for charged particle timing applications: performance after neutron irradiation
topic hep-ex
Particle Physics - Experiment
physics.ins-det
Detectors and Experimental Techniques
url https://dx.doi.org/10.1016/j.nima.2019.162930
http://cds.cern.ch/record/2653219
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