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56Fe(n,p)56Mn通常作为标准反应来监测中子场通量,该反应截面数据的准确性直接影响到活化法测量结果的精确度,进而影响到实验待测物理量的精度。本文开展了56Fe(n,p)56Mn反应截面实验测量数据评价工作与协方差计算工作,首先系统分析EXFOR中现有的56Fe(n,p)56Mn反应截面实验测量数据,对实验数据进行了归纳总结分析,并从中子源、测量方法、探测器类型等方面对56Fe(n,p)56Mn直接测量实验数据进行评价。然后,拟合给出适用入射中子能量区间为295~35 MeV的激发曲线。随后,针对评价中重点推荐的实验数据开展了关联协方差矩阵的计算工作。最后,使用核反应计算程序TALYS对56Fe(n,p)56Mn激发曲线进行了调参计算并和评价数据进行了比较分析。该工作拓展了现有的中子活化反应截面实验数据的评价方法,结果提高了35 MeV以下中子诱发56Fe(n,p)56Mn反应的评价数据精度。 相似文献
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Radiation shielding design of the CFETR polarimeter interferometer and CO2 dispersion interferometer
Bo HONG 《等离子体科学和技术》2022,24(6):64010
A three-wave based laser polarimeter/interferometer and a CO2 laser dispersion interferometer are used to determine the electron and current density profiles on a Chinese fusion engineering test reactor (CFETR). Radiation shielding is designed for the combination of polarimeter/interferometer and CO2 dispersion interferometer. Furthermore, neutronics models of the two systems are developed based on the engineering-integrated design of CFETR polarimeter/interferometer and CO2 dispersion interferometer and the major material components of CFETR. The polarimeter/interferometer and CO2 dispersion interferometer's neutron and photon transport simulations were performed using the Monte Carlo neutral transport code to determine the energy deposition and neutron energy spectrum of the optical mirrors. The energy depositions of the first mirrors on the polarimeter/interferometer are reduced by three orders with the whole shielding. Since the mirrors of CO2 dispersion interferometer are very close to the diagnostic first wall, shielding space is limited and the CO2 dispersion interferometer energy deposition is higher than that of the polarimeter/interferometer. The dose rate after shutdown 106 s in the back-drawer structure has been estimated to be 83 μSv h−1 when the radiation shield is filled in the diagnostic shielding modules, which is below the design threshold of 100 μSv h−1. Radiation shielding design plays a key role in successfully applying polarimeter/interferometer and CO2 dispersive interferometer in CFETR. 相似文献
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溴化镧(LaBr3:Ce)探测器是一种性能优良的无机闪烁体探测器,准确的LaBr3:Ce探测器γ响应参数以及响应能谱是开展应用工作的基础。通过对实验中实测γ能谱的分析,可以得到溴化镧谱仪的半高宽-能量关系,在尝试使用MCNP中GEB卡还原此关系时,发现可将程序中自带的半高宽-能量函数简化,简化后的函数关系仍能较好地反映实验测量信息。在此基础上,采用MCNP程序模拟了0.1~5 MeV的单能γ射线在Φ50 mm×10 mm溴化镧探测器中的响应输出,构建了其γ响应函数矩阵。通过能谱计算得到展宽系数后,编写MATLAB计算程序对构建的响应矩阵进行高斯展宽。利用展宽后的矩阵通过加权最小二乘法对实验测得的复杂能谱进行解谱,并将解谱结果与实验测量数据进行比较验证。结果表明:展宽后的响应函数与实验得到的响应函数符合一致,通过数值解谱可以很好地给出实验测量中不同γ源的能量以及相对产额等信息。 相似文献
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