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Measurements of the neutron spectra from the ~7Li(p,n) accelerator based neutron source: Position and angular dependences

机译:基于〜7Li(p,n)加速器的中子源的中子光谱测量:位置和角度依赖性

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Thick target ~7Li(p,n) neutron spectra were measured using a ~3He ion chamber in the proton energy range of 1.95 to 2.30 MeV. The fast neutron spectra were collected for various distances from the lithium target as well as for various neutron emission angles. By unfolding the ~3He raw data with the iterative van Cittert algorithm, the neutron fluence spectra were obtained. The ~3He measured neutron spectra were compared with both analytically computed and Monte Carlo simulated spectra to account for neutron scatterings in the lithium target assembly and in the experimental area. To verify the accuracy of the neutron dose computation, the fast neutron kerma was obtained for each neutron spectrum using the fluence to kerma conversion coefficients and was compared with the measured neutron dose using tissue-equivalent proportional counters. In the position dependence investigation at the 0° emission angle, the analytically computed neutron kerma overestimates the experimental kerma by a factor of two mainly due to neutron moderation. The corresponding neutron kerma from the ~3He measured spectra were in agreement with the neutron doses measured using tissue-equivalent proportional counters within 20% for lower proton energies, but the discrepancy increased to ~50% for higher proton energies. In the angular distribution investigation, a notable discrepancy between measured and computed neutron spectra were observed due to the neutron scattering effects in the target assembly and experimental room.
机译:使用〜3He离子室在质子能量为1.95至2.30 MeV的范围内测量了厚目标〜7Li(p,n)中子光谱。在距锂靶不同距离以及各种中子发射角度的情况下,收集了快中子光谱。通过用迭代范·切特算法展开〜3He原始数据,获得中子注量谱。将〜3He测量的中子光谱与分析计算的光谱和蒙特卡洛模拟的光谱进行比较,以说明锂靶组件和实验区域中的中子散射。为了验证中子剂量计算的准确性,使用注量到比释动能转换系数获得每个中子谱的快速中子比释动能,并使用组织当量比例计数器将其与测得的中子剂量进行比较。在0°发射角的位置相关性研究中,分析计算出的中子比释动能高估实验性比​​释动能两倍,这主要是由于中子减速所致。来自〜3He测量光谱的相应中子比释动能与使用组织当量比例计数器测量的中子剂量(质子能量较低)在20%以内,但质子能量较高的差异增加至〜50%。在角分布研究中,由于靶组件和实验室中的中子散射效应,观测到的中子光谱与计算出的中子光谱之间存在显着差异。

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