Cargando…
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...
Autores principales: | , , , , , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2018
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/j.nima.2019.162930 http://cds.cern.ch/record/2653219 |
_version_ | 1780961028734976000 |
---|---|
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. |
id | cern-2653219 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2018 |
record_format | invenio |
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 |
work_keys_str_mv | AT centisvignalim deepdiffusedapdsforchargedparticletimingapplicationsperformanceafterneutronirradiation AT gallinarom deepdiffusedapdsforchargedparticletimingapplicationsperformanceafterneutronirradiation AT harropb deepdiffusedapdsforchargedparticletimingapplicationsperformanceafterneutronirradiation AT luc deepdiffusedapdsforchargedparticletimingapplicationsperformanceafterneutronirradiation AT mcclishm deepdiffusedapdsforchargedparticletimingapplicationsperformanceafterneutronirradiation AT mollm deepdiffusedapdsforchargedparticletimingapplicationsperformanceafterneutronirradiation AT newcomerfm deepdiffusedapdsforchargedparticletimingapplicationsperformanceafterneutronirradiation AT oterougobonos deepdiffusedapdsforchargedparticletimingapplicationsperformanceafterneutronirradiation AT whites deepdiffusedapdsforchargedparticletimingapplicationsperformanceafterneutronirradiation |