Radiation shielding and safety implications following linac conversion to an electron FLASH‐RT unit

dc.contributor.authorPoirier, Yannick
dc.contributor.authorMossahebi, Sina
dc.contributor.authorBecker, Becker
dc.contributor.authorKoger, Brandon
dc.contributor.authorXu, Junliang
dc.contributor.authorLamichhane, Narrotam
dc.contributor.authorMaxim, Peter G.
dc.contributor.authorSawant, Amit
dc.contributor.departmentRadiation Oncology, School of Medicineen_US
dc.date.accessioned2022-02-04T22:27:58Z
dc.date.available2022-02-04T22:27:58Z
dc.date.issued2021-09
dc.description.abstractPurpose Due to their finite range, electrons are typically ignored when calculating shielding requirements in megavoltage energy linear accelerator vaults. However, the assumption that 16 MeV electrons need not be considered does not hold when operated at FLASH-RT dose rates (~200× clinical dose rate), where dose rate from bremsstrahlung photons is an order of magnitude higher than that from an 18 MV beam for which shielding was designed. We investigate the shielding and radiation protection impact of converting a Varian 21EX linac to FLASH-RT dose rates. Methods We performed a radiation survey in all occupied areas using a Fluke Biomedical Inovision 451P survey meter and a Wide Energy Neutron Detection Instrument (Wendi)-2 FHT 762 neutron detector. The dose rate from activated linac components following a 1.8-min FLASH-RT delivery was also measured. Results When operated at a gantry angle of 180° such as during biology experiments, the 16 MeV FLASH-RT electrons deliver ~10 µSv/h in the controlled areas and 780 µSv/h in the uncontrolled areas, which is above the 20 µSv in any 1-h USNRC limit. However, to exceed 20 µSv, the unit must be operated continuously for 92 s, which corresponds in this bunker and FLASH-RT beam to a 3180 Gy workload at isocenter, which would be unfeasible to deliver within that timeframe due to experimental logistics. While beam steering and dosimetry activities can require workloads of that magnitude, during these activities, the gantry is positioned at 0° and the dose rate in the uncontrolled area becomes undetectable. Likewise, neutron activation of linac components can reach 25 µSv/h near the isocenter following FLASH-RT delivery, but dissipates within minutes, and total doses within an hour are below 20 µSv. Conclusion Bremsstrahlung photons created by a 16 MeV FLASH-RT electron beam resulted in consequential dose rates in controlled and uncontrolled areas, and from activated linac components in the vault. While our linac vault shielding proved sufficient, other investigators would be prudent to confirm the adequacy of their radiation safety program, particularly if operating in vaults designed for 6 MV.en_US
dc.eprint.versionAuthor's manuscripten_US
dc.identifier.citationPoirier, Y., Mossahebi, S., Becker, S. J., Koger, B., Xu, J., Lamichhane, N., Maxim, P. G., & Sawant, A. (2021). Radiation shielding and safety implications following linac conversion to an electron FLASH‐RT unit. Medical Physics, 48(9), 5396–5405. https://doi.org/10.1002/mp.15105en_US
dc.identifier.issn5396-5405en_US
dc.identifier.urihttps://hdl.handle.net/1805/27711
dc.language.isoen_USen_US
dc.publisherAmerican Association of Physicists in Medicneen_US
dc.relation.isversionof10.1002/mp.15105en_US
dc.relation.journalMedical Physicsen_US
dc.rightsPublisher Policyen_US
dc.sourceAuthoren_US
dc.subjectelectronsen_US
dc.subject16 MeV electronsen_US
dc.subjectradiation surveyen_US
dc.subjectlinac conversionen_US
dc.titleRadiation shielding and safety implications following linac conversion to an electron FLASH‐RT uniten_US
dc.typeArticleen_US
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