用蒙特卡洛法估算邦纳球串扰并用 241Am-Be 中子源校准光谱仪

IF 1.5 3区 物理与天体物理 Q3 INSTRUMENTS & INSTRUMENTATION
Hai Wan, Luying Yang, Xiaofei Jiang
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引用次数: 0

摘要

使用邦纳球谱仪(BSS)进行中子谱测量通常有两种实验方法。一种是每次只使用一个邦纳球(BS),通过反复测量完成中子实验;另一种是多个邦纳球(BS)一起测量,这种多球同时测量的方法只能完成一次中子实验。单球测量法无法保证每次测量环境都完全一致,因此不可避免地会产生测量误差。多球同时测量法可以保证每个球的实验环境相同,但会产生串扰。本文研究了串扰对 BSS 的影响。首先,我们利用 Geant4 模拟了有串扰和无串扰时相应的中子响应函数,并分析了两种中子响应函数之间的误差。其次,模拟中子源实验的中子计数。考虑到 BSS 靠近地板,计算了有无串扰和地板散射时 BS 的中子计数误差。最后,我们使用 BSS 实际测量了中子源,获得了 8 个中子计数。通过校准串扰的影响,得到了中子源的频谱。结果表明,影响 BS 计数的散裂中子主要是原初散裂中子,占所有散裂中子的 90% 以上。散裂中子主要影响高能域大 BS 和低能域小 BS 的中子响应函数。串扰对大型和小型 BS 的中子计数都有很大影响,而地板散射只对小型 BS 有很大影响。校准中子计数得到的中子谱比原始实验计数得到的中子谱更精确。特别是在 1~5 MeV 范围内,校准中子谱更接近国际标准谱。校准中子谱的均方误差(RMSE)降低了 3.86%。本文通过分析串扰的影响,对BSS的中子计数进行了标定,提高了中子谱的精度,为展开中子谱提供了有力的依据。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Estimation of Bonner sphere cross-talking with Monte Carlo method and spectrometer calibration with 241Am-Be neutron source
There are usually two kinds of experiment methods for neutron spectrum measurement by Bonner sphere spectrometer (BSS). The first is to use only one Bonner sphere (BS) at a time to complete the neutron experiment by repeated measurements; The other is to measure multiple Bonner spheres (BSs) together, and this multi-sphere simultaneous measurement method can complete the neutron experiment only once. The single sphere measurement method cannot guarantee that the measurement environment is completely consistent every time, which leads to inevitable measurement errors. The multi-sphere simultaneous measurement method can ensure the same experimental environment for each sphere, but there will be cross-talking. This paper studies the influence of cross-talking on BSS. Firstly, we use Geant4 to simulate the corresponding neutron response function with and without cross-talking, and analyze the error between the two neutron response functions. Secondly, the neutron count of
neutron source experiment is simulated. Considering that the BSS is close to the floor, the neutron counting error of BS with and without cross-talking and floor scattering is calculated. Finally, we actually measure the
neutron source using a BSS and obtain 8 neutron counts. The spectrum of
neutron source is obtained by calibrating the influence of cross-talking. The results show that the scattered neutrons which affect the count of BS are mainly the primary scattered neutrons, which account for more than 90% of all scattered neutrons. The scattered neutrons mainly affect the neutron response function of the large BS in the high energy domain and the small BS in the low energy domain. The cross-talking has a great influence on the neutron count of large and small BS, while the floor scattering has a great influence only on the small BS. The
neutron spectrum obtained by calibrated neutron counts is more accurate than that obtained by the original experiment counts. Especially in the range of 15 MeV, the calibrated
neutron spectrum is much closer to the international standard spectrum. The mean square error (RMSE) of calibrated
neutron spectrum is reduced by 3.86%. In this paper, by analyzing the influence of cross-talking, the neutron count of BSS is calibrated, and the accuracy of
neutron spectrum is improved, which provides a strong basis for unfolding neutron spectrum.
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来源期刊
CiteScore
3.20
自引率
21.40%
发文量
787
审稿时长
1 months
期刊介绍: Section A of Nuclear Instruments and Methods in Physics Research publishes papers on design, manufacturing and performance of scientific instruments with an emphasis on large scale facilities. This includes the development of particle accelerators, ion sources, beam transport systems and target arrangements as well as the use of secondary phenomena such as synchrotron radiation and free electron lasers. It also includes all types of instrumentation for the detection and spectrometry of radiations from high energy processes and nuclear decays, as well as instrumentation for experiments at nuclear reactors. Specialized electronics for nuclear and other types of spectrometry as well as computerization of measurements and control systems in this area also find their place in the A section. Theoretical as well as experimental papers are accepted.
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