Pinto M, Bajard M, Brons S, Chevallier M, Dauvergne D, Dedes G, De Rydt M, Freud N, Krimmer J, La Tessa C, Létang J M, Parodi K, Pleskač R, Prieels D, Ray C, Rinaldi I, Roellinghoff F, Schardt D, Testa E, Testa M
IPNL; Université de Lyon, F-69003 Lyon, France; Université Lyon 1, F-69622 Villeurbanne, France; CNRS/IN2P3, UMR 5822 F-69622 Villeurbanne, France.
Phys Med Biol. 2015 Jan 21;60(2):565-94. doi: 10.1088/0031-9155/60/2/565. Epub 2014 Dec 30.
Prompt-gamma emission detection is a promising technique for hadrontherapy monitoring purposes. In this regard, obtaining prompt-gamma yields that can be used to develop monitoring systems based on this principle is of utmost importance since any camera design must cope with the available signal. Herein, a comprehensive study of the data from ten single-slit experiments is presented, five consisting in the irradiation of either PMMA or water targets with lower and higher energy carbon ions, and another five experiments using PMMA targets and proton beams. Analysis techniques such as background subtraction methods, geometrical normalization, and systematic uncertainty estimation were applied to the data in order to obtain absolute prompt-gamma yields in units of prompt-gamma counts per incident ion, unit of field of view, and unit of solid angle. At the entrance of a PMMA target, where the contribution of secondary nuclear reactions is negligible, prompt-gamma counts per incident ion, per millimetre and per steradian equal to (124 ± 0.7stat ± 30sys) × 10(-6) for 95 MeV u(-1) carbon ions, (79 ± 2stat ± 23sys) × 10(-6) for 310 MeV u(-1) carbon ions, and (16 ± 0.07stat ± 1sys) × 10(-6) for 160 MeV protons were found for prompt gammas with energies higher than 1 MeV. This shows a factor 5 between the yields of two different ions species with the same range in water (160 MeV protons and 310 MeV u(-1) carbon ions). The target composition was also found to influence the prompt-gamma yield since, for 300/310 MeV u(-1) carbon ions, a 42% greater yield ((112 ± 1stat ± 22sys) × 10(-6) counts ion(-1) mm(-1) sr(-1)) was obtained with a water target compared to a PMMA one.
瞬发伽马发射探测是一种很有前景的用于强子治疗监测的技术。在这方面,获取可用于基于此原理开发监测系统的瞬发伽马产额至关重要,因为任何相机设计都必须应对可用信号。本文展示了对十个单缝实验数据的全面研究,其中五个实验是用较低和较高能量的碳离子照射聚甲基丙烯酸甲酯(PMMA)或水靶,另外五个实验使用PMMA靶和质子束。为了获得以每入射离子的瞬发伽马计数、视场单位和立体角单位为单位的绝对瞬发伽马产额,对数据应用了诸如背景扣除方法、几何归一化和系统不确定度估计等分析技术。在PMMA靶的入口处,二次核反应的贡献可忽略不计,对于能量高于1 MeV的瞬发伽马,每入射离子、每毫米和每球面度的瞬发伽马计数对于95 MeV u⁻¹的碳离子等于(124 ± 0.7统计 ± 30系统)×10⁻⁶,对于310 MeV u⁻¹的碳离子等于(79 ± 2统计 ± 23系统)×10⁻⁶,对于160 MeV的质子等于(16 ± 0.07统计 ± 1系统)×10⁻⁶。这表明在水中具有相同射程的两种不同离子种类(160 MeV质子和310 MeV u⁻¹碳离子)的产额之间存在5倍的差异。还发现靶的成分会影响瞬发伽马产额,因为对于300/310 MeV u⁻¹的碳离子,与PMMA靶相比,水靶获得的产额高42%((112 ± 1统计 ± 22系统)×10⁻⁶计数离子⁻¹毫米⁻¹球面度⁻¹)。