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基于前冲康普顿电子高能伽马能谱测量系统设计
引用本文:贾清刚,张天奎,许海波.基于前冲康普顿电子高能伽马能谱测量系统设计[J].物理学报,2017,66(1):10703-010703.
作者姓名:贾清刚  张天奎  许海波
作者单位:1. 中国工程物理研究院北京应用物理与计算数学研究所, 北京 100094;2. 中国工程物理研究院激光聚变研究中心, 绵阳 621900
基金项目:中国博士后科学基金(批准号:2015M581028)、国家自然基金(批准号:11675021,11505166)和中国工程物理研究院科学技术发展基金(批准号:2014A0402016)资助的课题.
摘    要:除中子外,聚变核心同时释放大量高能伽马,其能谱可反映聚变过程的关键物理参数,并为过程诊断提供重要信息.由于聚变伽马的时间与能量特性,需要设计高探测效率及能量分辨率的伽马谱仪.根据高能伽马谱仪的概念设计(gamma-to-electron magnetic spectrometer),针对该系统中伽马-电子转换靶、电子偏转汇聚、电子探测等关键环节进行优化设计以提高系统探测效率及能量分辨率.其中采用Monte-Carlo程序Geant4模拟研究了伽马-电子转换靶中康普顿散射与多次库仑散射对由转换靶出射电子的能谱与角分布的影响.开发并行遗传算法对复杂几何偏转磁场参数进行优化,得到低强度(小于100 Gauss)复杂边界偏转磁场.根据系统优化设计结果,采用Geant4模拟了该系统对不同能量伽马的响应.此外,还可模拟该系统对特征聚变伽马能谱的测量,结果显示,该系统可在聚变中子产额分别为2.5×10~(15)及1.2×10~(16)条件下,对10—20 MeV高能伽马能谱测量实现能量分辨分别满足0.5 MeV(小于5%)及0.25 MeV(小于2.5%),说明该系统可用于聚变过程伽马能谱的诊断.

关 键 词:能谱测量  聚变伽马射线  磁偏转系统  Geant4
收稿时间:2016-07-03

Optimization design of a Gamma-to-electron spectrometer for high energy gammas induced by fusion
Jia Qing-Gang,Zhang Tian-Kui,Xu Hai-Bo.Optimization design of a Gamma-to-electron spectrometer for high energy gammas induced by fusion[J].Acta Physica Sinica,2017,66(1):10703-010703.
Authors:Jia Qing-Gang  Zhang Tian-Kui  Xu Hai-Bo
Institution:1. Institute of Applied Physics and Computational Mathematics, Beijing 100094, China;2. Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China
Abstract:Apart from neutrons, the fusion core produces gamma rays during fusion reaction. The spectrum of gamma ray can provide very important information for fusion diagnosis. However, due to the gamma energy and yield in one fusion pulse being both lower, the gamma spectrometer used should have high detection efficiency and energy resolution. The concept of a Gamma-to-electron magnetic spectrometer(GEMS) provides the idea to build up such a spectrometer to meet this requirement. Based on this concept design, four important parts of this facility are investigated. The first part is the gamma-electron converter. The main physics processes include Compton scattering of gamma ray with converter material generating electron, the electron multiple Coulomb scattering(MCS) inside the converter and the electron attenuation. Affected by the thickness of convector, these processes give a complex influence on the detection efficiency and angular-energy distribution of the electrons which are emitted from the downstream face of the convector. The Monte Carlo code Geant4 is employed to investigate theeffects of Compton scattering, MCS and converter thick on the angular-energy distribution. The second one is the collimation. The collimation is used to select the forward direction, the performances of cutoff angle of the collimator on the detection efficiency and resolutions, the correlation between electron transportation direction and energy, are also studied using Geant4 code. The third part is the dipole magnetic field. There are several geometric and magnetic parameters, therefore, a multi-thread parallelized genetic algorithm is developed to obtain the best result. Both the irregular geometric shape and dipole magnetic field strength are optimized to achieve the best energy resolution and detection efficiency. The obtained magnetic field has an intensity of less than 100 Gauss, and its performance on gathering elections is also verified by Geant4 code. The last one is the location of electron detectors. The study shows that all the electron detectors should be located not in a straight line but a quadratic curve. Then the optimized spectrometer is simulated by Geant4 to obtain the responses of gamma rays with various energies. For the gammas provided by fusion reaction, the simulation shows that when the neutron yields are about 2.5×1015 and 1.2×1016, the energy resolutions reach 0.5 MeV and 0.25 MeV, respectively, provided that different thick Be converters are employed. All in all, this optimized GEMS can be employed to measure the spectrum of gamma rays generated fom the fusion reaction.
Keywords:spectrometer  fusion gamma ray  dipole  Geant4
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