Cargando…
Irradiation effects on Gd$_{3}$AI$_{3}$Ga$_{3}$O$_{12}$ scintillators prospective for application in harsh irradiation environments
We provide evidences that multicomponent garnet-type Ce-doped crystal GAGG (Gd$_{3}$AI$_{3}$Ga$_{3}$O$_{12}$) is a promising scintillator to be applied in harsh irradiation environments, particularly, in high-energy physics experiments and reactor research facilities, where long-term operation is ma...
Autores principales: | , , , , , , , , , , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2019
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/j.radphyschem.2019.108365 http://cds.cern.ch/record/2801576 |
_version_ | 1780972706127151104 |
---|---|
author | Auffray, E Dosovitskiy, G Fedorov, A Guz, I Korjik, M Kratochwill, N Lucchini, M Nargelas, S Kozlov, D Mechinsky, V Orsich, P Sidletskiy, O Tamulaitis, G Vaitkevičius, A |
author_facet | Auffray, E Dosovitskiy, G Fedorov, A Guz, I Korjik, M Kratochwill, N Lucchini, M Nargelas, S Kozlov, D Mechinsky, V Orsich, P Sidletskiy, O Tamulaitis, G Vaitkevičius, A |
author_sort | Auffray, E |
collection | CERN |
description | We provide evidences that multicomponent garnet-type Ce-doped crystal GAGG (Gd$_{3}$AI$_{3}$Ga$_{3}$O$_{12}$) is a promising
scintillator to be applied in harsh irradiation environments, particularly, in high-energy physics experiments and
reactor research facilities, where long-term operation is mandatory. Applicability of this scintillator for the
upgrade of the detectors at future accelerators with high luminosity like High luminosity LHC is considered and
GAGG:Ce with different codopings is compared with Ce-doped oxyorthosilicate crystals, which are currently also
strong candidates for such applications. It is shown that the irradiation with 24 GeV protons at a fluence of
$5 \times 10^{14}$ p/cm$^2$ has no significant effect on optical absorption in the spectral range of the scintillator emission. The
contribution of radioisotopes formed in the material by irradiation with protons to the noise pedestal and the
noise energy equivalent due to harmful radio-luminescence excited by the radionuclides remains negligible at
short gates in collider experiments. Moreover, we show that the irradiation-generated color centers absorb
outside the spectral range of Ce luminescence. These centers do not significantly affect the dynamics of nonequilibrium carriers, which is responsible for the timing properties of the scintillator. The density of free carriers
decays with a characteristic time of 2 ps, while the decay constant for trapped carriers is ∼50 ns both before and
after irradiation. |
id | cern-2801576 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2019 |
record_format | invenio |
spelling | cern-28015762022-10-28T12:12:39Zdoi:10.1016/j.radphyschem.2019.108365http://cds.cern.ch/record/2801576engAuffray, EDosovitskiy, GFedorov, AGuz, IKorjik, MKratochwill, NLucchini, MNargelas, SKozlov, DMechinsky, VOrsich, PSidletskiy, OTamulaitis, GVaitkevičius, AIrradiation effects on Gd$_{3}$AI$_{3}$Ga$_{3}$O$_{12}$ scintillators prospective for application in harsh irradiation environmentsNuclear Physics - ExperimentWe provide evidences that multicomponent garnet-type Ce-doped crystal GAGG (Gd$_{3}$AI$_{3}$Ga$_{3}$O$_{12}$) is a promising scintillator to be applied in harsh irradiation environments, particularly, in high-energy physics experiments and reactor research facilities, where long-term operation is mandatory. Applicability of this scintillator for the upgrade of the detectors at future accelerators with high luminosity like High luminosity LHC is considered and GAGG:Ce with different codopings is compared with Ce-doped oxyorthosilicate crystals, which are currently also strong candidates for such applications. It is shown that the irradiation with 24 GeV protons at a fluence of $5 \times 10^{14}$ p/cm$^2$ has no significant effect on optical absorption in the spectral range of the scintillator emission. The contribution of radioisotopes formed in the material by irradiation with protons to the noise pedestal and the noise energy equivalent due to harmful radio-luminescence excited by the radionuclides remains negligible at short gates in collider experiments. Moreover, we show that the irradiation-generated color centers absorb outside the spectral range of Ce luminescence. These centers do not significantly affect the dynamics of nonequilibrium carriers, which is responsible for the timing properties of the scintillator. The density of free carriers decays with a characteristic time of 2 ps, while the decay constant for trapped carriers is ∼50 ns both before and after irradiation.oai:cds.cern.ch:28015762019 |
spellingShingle | Nuclear Physics - Experiment Auffray, E Dosovitskiy, G Fedorov, A Guz, I Korjik, M Kratochwill, N Lucchini, M Nargelas, S Kozlov, D Mechinsky, V Orsich, P Sidletskiy, O Tamulaitis, G Vaitkevičius, A Irradiation effects on Gd$_{3}$AI$_{3}$Ga$_{3}$O$_{12}$ scintillators prospective for application in harsh irradiation environments |
title | Irradiation effects on Gd$_{3}$AI$_{3}$Ga$_{3}$O$_{12}$ scintillators prospective for application in harsh irradiation environments |
title_full | Irradiation effects on Gd$_{3}$AI$_{3}$Ga$_{3}$O$_{12}$ scintillators prospective for application in harsh irradiation environments |
title_fullStr | Irradiation effects on Gd$_{3}$AI$_{3}$Ga$_{3}$O$_{12}$ scintillators prospective for application in harsh irradiation environments |
title_full_unstemmed | Irradiation effects on Gd$_{3}$AI$_{3}$Ga$_{3}$O$_{12}$ scintillators prospective for application in harsh irradiation environments |
title_short | Irradiation effects on Gd$_{3}$AI$_{3}$Ga$_{3}$O$_{12}$ scintillators prospective for application in harsh irradiation environments |
title_sort | irradiation effects on gd$_{3}$ai$_{3}$ga$_{3}$o$_{12}$ scintillators prospective for application in harsh irradiation environments |
topic | Nuclear Physics - Experiment |
url | https://dx.doi.org/10.1016/j.radphyschem.2019.108365 http://cds.cern.ch/record/2801576 |
work_keys_str_mv | AT auffraye irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT dosovitskiyg irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT fedorova irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT guzi irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT korjikm irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT kratochwilln irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT lucchinim irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT nargelass irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT kozlovd irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT mechinskyv irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT orsichp irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT sidletskiyo irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT tamulaitisg irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments AT vaitkeviciusa irradiationeffectsongd3ai3ga3o12scintillatorsprospectiveforapplicationinharshirradiationenvironments |