2020
DOI: 10.1016/j.nima.2020.164364
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TOF diagnosis of laser accelerated, high-energy protons

Abstract: Significant challenges in the detection of laser-accelerated ions result from the high flux (10 10 -10 12 ions/pulse) and the short bunch duration which are intrinsic to laser-driven sources. The development of diagnostic techniques able to operate in real-time and on a high-rep basis is a key step towards multidisciplinary applications of such non-conventional beams. Real time diagnosis of the main beam parameters for high-energy protons accelerated by the Vulcan Petawatt (VULCAN-PW) laser system has been per… Show more

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Cited by 16 publications
(11 citation statements)
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“…The TPS and the RCF are usually placed along the target-normal direction to measure the higher-energy component and used for the full beam characterization in advance of the cell irradiations. In contrast, TOF detectors (typically diamond and silicon carbide) [52,53] can be placed at various angles both in the forward and backward directions to monitor the particle flux and energy on-line during the irradiation, and detect any shot-to-shot variations [54]. A crucial task in view of meaningful radiobiological investigations is a precise measurement of the dose delivered to the cells.…”
Section: Diagnostics and Dosimetrymentioning
confidence: 99%
“…The TPS and the RCF are usually placed along the target-normal direction to measure the higher-energy component and used for the full beam characterization in advance of the cell irradiations. In contrast, TOF detectors (typically diamond and silicon carbide) [52,53] can be placed at various angles both in the forward and backward directions to monitor the particle flux and energy on-line during the irradiation, and detect any shot-to-shot variations [54]. A crucial task in view of meaningful radiobiological investigations is a precise measurement of the dose delivered to the cells.…”
Section: Diagnostics and Dosimetrymentioning
confidence: 99%
“…After exiting the vacuum chamber, the bunch travels through an air gap of 6.5 cm in length. Then, the proton bunch passes either an aperture equipped with a timeof-flight (TOF) spectrometer [11,19,20] and a parallel plate ionization chamber (IC, X-Ray Therapy Monitor Chamber 7862, PTW Freiburg) positioned behind the aperture connected to a dosemeter (UNIDOS, PTW Freiburg) to deduce the proton bunch particle number or a collimator of variable diameter between 1 and 5 mm. The bunch then enters the I-BEAT 3D detector which is positioned 8 cm behind the aperture or the collimator, respectively.…”
Section: Experimental Set-upmentioning
confidence: 99%
“…On the other hand, if they had a longer range, they would cross the whole body of the detector releasing just a portion of their energy in it. In the latter case, the deposited energy does not correspond to the one possessed by the particle itself and estimated thanks to equation (2.1), thus equation (2.2) has to be corrected by a proper factor [17,18].…”
Section: High Energy Correction Factormentioning
confidence: 99%