2019
DOI: 10.1016/j.radonc.2019.05.004
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Dosimetric and preparation procedures for irradiating biological models with pulsed electron beam at ultra-high dose-rate

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Cited by 106 publications
(135 citation statements)
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“…The roles of dose-per-pulse, instantaneous dose per pulse (dose per pulse divided by pulse duration), and pulse duration and frequency still remain to be understood. This is essentially due to the fact that the accelerators used up to now for in vivo FLASH experiments are electron accelerators designed for industrial use [18][19][20] or modified medical accelerators, where diffuser filters and monitor chambers have been mechanically dismounted and removed from the beam path [21]. Therefore, such accelerators are not able to perform beam parameters real-time monitoring as well as provide an accurate and reproducible output.…”
Section: Introductionmentioning
confidence: 99%
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“…The roles of dose-per-pulse, instantaneous dose per pulse (dose per pulse divided by pulse duration), and pulse duration and frequency still remain to be understood. This is essentially due to the fact that the accelerators used up to now for in vivo FLASH experiments are electron accelerators designed for industrial use [18][19][20] or modified medical accelerators, where diffuser filters and monitor chambers have been mechanically dismounted and removed from the beam path [21]. Therefore, such accelerators are not able to perform beam parameters real-time monitoring as well as provide an accurate and reproducible output.…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, the dosimetry is complicated by the saturation problems typical of all clinical dosimeters which provide online information to these dose-per-pulse values. In all the experimental works published so far [18][19][20][21], the dosimetry was performed using independent dose-rate dosimeters, in most cases radiochromic films. Radiochromic films do not have the same accuracy of other detectors (for example ionization chambers), they do not provide online dosimetric information, and they are not able to control any changes in the output during the experiment.…”
Section: Introductionmentioning
confidence: 99%
“…Irradiation was performed using a prototype 6 MeV electron beam, LINAC, of the Oriatron type 6e (eRT6; PMB Alcen), available at Lausanne University Hospital and described previously [62]. Physical dosimetry has been extensively described and published to ensure reproducible and reliable biological studies [13,[63][64][65]. This LINAC was able to produce a pulsed electron beam at a mean dose rate ranging from 0.1 Gy/s (i.e., comparable to CONV used in RT) up to 4.4 × 10 6 Gy/s (at standard distance), corresponding to a dose, in each electron pulse, ranging from 0.01 up to 8 Gy.…”
Section: Whole Brain Irradiationsmentioning
confidence: 99%
“…on the dose-rate, which is the quantity to be measured. Although specific models have been recently developed to characterize the saturation and compute the absolute dose, this saturation effect may vary depending on the beam characteristics and irradiation setup, which makes the establishment of the correction factors inaccurate and time-consuming [13]. Additionally, ionization chambers need several tens of µs (30-300 µs for 0.5-5 mm air gap) to collect the charges and are too slow to monitor a FLASH beam, which delivers tens of Gy in a few µs.…”
Section: Beam Monitors In Conventional Radiotherapymentioning
confidence: 99%