Monitoring of Ultra-High Dose Rate Pulsed X-ray Facilities with Radioluminescent Nitrogen-Doped Optical Fiber
We exploited the potential of radiation-induced emissions (RIEs) in the visible domain of a nitrogen-doped, silica-based, multimode optical fiber to monitor the very high dose rates associated with experiments at different pulsed X-ray facilities. We also tested this sensor at lower dose rates assoc...
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MDPI AG
2022-04-01
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Online Access: | https://www.mdpi.com/1424-8220/22/9/3192 |
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author | Jeoffray Vidalot Cosimo Campanella Julien Dachicourt Claude Marcandella Olivier Duhamel Adriana Morana David Poujols Gilles Assaillit Marc Gaillardin Aziz Boukenter Youcef Ouerdane Sylvain Girard Philippe Paillet |
author_facet | Jeoffray Vidalot Cosimo Campanella Julien Dachicourt Claude Marcandella Olivier Duhamel Adriana Morana David Poujols Gilles Assaillit Marc Gaillardin Aziz Boukenter Youcef Ouerdane Sylvain Girard Philippe Paillet |
author_sort | Jeoffray Vidalot |
collection | DOAJ |
description | We exploited the potential of radiation-induced emissions (RIEs) in the visible domain of a nitrogen-doped, silica-based, multimode optical fiber to monitor the very high dose rates associated with experiments at different pulsed X-ray facilities. We also tested this sensor at lower dose rates associated with steady-state X-ray irradiation machines (up to 100 keV photon energy, mean energy of 40 keV). For transient exposures, dedicated experimental campaigns were performed at ELSA (Electron et Laser, Source X et Applications) and ASTERIX facilities from CEA (Commissariat à l’Energie Atomique—France) to characterize the RIE of this fiber when exposed to X-ray pulses with durations of a few µs or ns. These facilities provide very large dose rates: in the order of MGy(SiO<sub>2</sub>)/s for the ELSA facility (up to 19 MeV photon energy) and GGy(SiO<sub>2</sub>)/s for the ASTERIX facility (up to 1 MeV). In both cases, the RIE intensities, mostly explained by the fiber radioluminescence (RIL) around 550 nm, with a contribution from Cerenkov at higher fluxes, linearly depend on the dose rates normalized to the pulse duration delivered by the facilities. By comparing these high dose rate results and those acquired under low-dose rate steady-state X-rays (only RIL was present), we showed that the RIE of this multimode optical fiber linearly depends on the dose rate over an ultra-wide dose rate range from 10<sup>−2</sup> Gy(SiO<sub>2</sub>)/s to a few 10<sup>9</sup> Gy(SiO<sub>2</sub>)/s and photons with energy in the range from 40 keV to 19 MeV. These results demonstrate the high potential of this class of radiation monitors for beam monitoring at very high dose rates in a very large variety of facilities as future FLASH therapy facilities. |
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language | English |
last_indexed | 2024-03-10T03:42:55Z |
publishDate | 2022-04-01 |
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spelling | doaj.art-58ad5c9a30274b5d860b7e9d1fb60c9e2023-11-23T09:14:47ZengMDPI AGSensors1424-82202022-04-01229319210.3390/s22093192Monitoring of Ultra-High Dose Rate Pulsed X-ray Facilities with Radioluminescent Nitrogen-Doped Optical FiberJeoffray Vidalot0Cosimo Campanella1Julien Dachicourt2Claude Marcandella3Olivier Duhamel4Adriana Morana5David Poujols6Gilles Assaillit7Marc Gaillardin8Aziz Boukenter9Youcef Ouerdane10Sylvain Girard11Philippe Paillet12Commissariat à l’Energie Atomique et aux Energies Alternatives (CEA), Direction des Applications Militaires (DAM-DIF), F-91297 Arpajon, FranceLaboratoire Hubert Curien, Université Jean Monnet, CNRS 5516, IOGS, F-42000 Saint Etienne, FranceCommissariat à l’Energie Atomique et aux Energies Alternatives (CEA), Direction des Applications Militaires (DAM-DIF), F-91297 Arpajon, FranceCommissariat à l’Energie Atomique et aux Energies Alternatives (CEA), Direction des Applications Militaires (DAM-DIF), F-91297 Arpajon, FranceCommissariat à l’Energie Atomique et aux Energies Alternatives (CEA), Direction des Applications Militaires (DAM-DIF), F-91297 Arpajon, FranceLaboratoire Hubert Curien, Université Jean Monnet, CNRS 5516, IOGS, F-42000 Saint Etienne, FranceCentre d’Etudes de Gramat (CEG), Commissariat à l’Energie Atomique et aux Energies Alternatives (CEA), F-46500 Gramat, FranceCentre d’Etudes de Gramat (CEG), Commissariat à l’Energie Atomique et aux Energies Alternatives (CEA), F-46500 Gramat, FranceCentre d’Etudes de Gramat (CEG), Commissariat à l’Energie Atomique et aux Energies Alternatives (CEA), F-46500 Gramat, FranceLaboratoire Hubert Curien, Université Jean Monnet, CNRS 5516, IOGS, F-42000 Saint Etienne, FranceLaboratoire Hubert Curien, Université Jean Monnet, CNRS 5516, IOGS, F-42000 Saint Etienne, FranceLaboratoire Hubert Curien, Université Jean Monnet, CNRS 5516, IOGS, F-42000 Saint Etienne, FranceCommissariat à l’Energie Atomique et aux Energies Alternatives (CEA), Direction des Applications Militaires (DAM-DIF), F-91297 Arpajon, FranceWe exploited the potential of radiation-induced emissions (RIEs) in the visible domain of a nitrogen-doped, silica-based, multimode optical fiber to monitor the very high dose rates associated with experiments at different pulsed X-ray facilities. We also tested this sensor at lower dose rates associated with steady-state X-ray irradiation machines (up to 100 keV photon energy, mean energy of 40 keV). For transient exposures, dedicated experimental campaigns were performed at ELSA (Electron et Laser, Source X et Applications) and ASTERIX facilities from CEA (Commissariat à l’Energie Atomique—France) to characterize the RIE of this fiber when exposed to X-ray pulses with durations of a few µs or ns. These facilities provide very large dose rates: in the order of MGy(SiO<sub>2</sub>)/s for the ELSA facility (up to 19 MeV photon energy) and GGy(SiO<sub>2</sub>)/s for the ASTERIX facility (up to 1 MeV). In both cases, the RIE intensities, mostly explained by the fiber radioluminescence (RIL) around 550 nm, with a contribution from Cerenkov at higher fluxes, linearly depend on the dose rates normalized to the pulse duration delivered by the facilities. By comparing these high dose rate results and those acquired under low-dose rate steady-state X-rays (only RIL was present), we showed that the RIE of this multimode optical fiber linearly depends on the dose rate over an ultra-wide dose rate range from 10<sup>−2</sup> Gy(SiO<sub>2</sub>)/s to a few 10<sup>9</sup> Gy(SiO<sub>2</sub>)/s and photons with energy in the range from 40 keV to 19 MeV. These results demonstrate the high potential of this class of radiation monitors for beam monitoring at very high dose rates in a very large variety of facilities as future FLASH therapy facilities.https://www.mdpi.com/1424-8220/22/9/3192radiation effectsoptical materialsradioluminescenceoptical fibersX-raysbeam monitoring |
spellingShingle | Jeoffray Vidalot Cosimo Campanella Julien Dachicourt Claude Marcandella Olivier Duhamel Adriana Morana David Poujols Gilles Assaillit Marc Gaillardin Aziz Boukenter Youcef Ouerdane Sylvain Girard Philippe Paillet Monitoring of Ultra-High Dose Rate Pulsed X-ray Facilities with Radioluminescent Nitrogen-Doped Optical Fiber Sensors radiation effects optical materials radioluminescence optical fibers X-rays beam monitoring |
title | Monitoring of Ultra-High Dose Rate Pulsed X-ray Facilities with Radioluminescent Nitrogen-Doped Optical Fiber |
title_full | Monitoring of Ultra-High Dose Rate Pulsed X-ray Facilities with Radioluminescent Nitrogen-Doped Optical Fiber |
title_fullStr | Monitoring of Ultra-High Dose Rate Pulsed X-ray Facilities with Radioluminescent Nitrogen-Doped Optical Fiber |
title_full_unstemmed | Monitoring of Ultra-High Dose Rate Pulsed X-ray Facilities with Radioluminescent Nitrogen-Doped Optical Fiber |
title_short | Monitoring of Ultra-High Dose Rate Pulsed X-ray Facilities with Radioluminescent Nitrogen-Doped Optical Fiber |
title_sort | monitoring of ultra high dose rate pulsed x ray facilities with radioluminescent nitrogen doped optical fiber |
topic | radiation effects optical materials radioluminescence optical fibers X-rays beam monitoring |
url | https://www.mdpi.com/1424-8220/22/9/3192 |
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