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1.中国工程物理研究院 材料研究所表面物理与化学重点实验室 江油 621907;
2.中国工程物理研究院材料研究所 绵阳 621700
王亭亭,女,1990年出生,2013年毕业于中国科学技术大学,现为硕士研究生,辐射防护与环境保护专业
熊忠华,E-mail:xiongzhonghua@caep.cn
收稿日期:2015-10-15,
录用日期:2016-03-15,
纸质出版日期:2016-01-25
移动端阅览
王亭亭, 王亮, 莫钊洪, 等. EJ339A型液体闪烁探测系统光输出响应函数的理论模拟与实验研究[J]. 核技术, 2016,39(5):050403
Tingting WANG, Liang WANG, Zhaohong MO, et al. Theoretical simulation and experimental research of the light output function of liquid scintillator EJ339A[J]. Nuclear techniques, 2016, 39(5): 050403
王亭亭, 王亮, 莫钊洪, 等. EJ339A型液体闪烁探测系统光输出响应函数的理论模拟与实验研究[J]. 核技术, 2016,39(5):050403 DOI: 10.11889/j.0253-3219.2016.hjs.39.050403.
Tingting WANG, Liang WANG, Zhaohong MO, et al. Theoretical simulation and experimental research of the light output function of liquid scintillator EJ339A[J]. Nuclear techniques, 2016, 39(5): 050403 DOI: 10.11889/j.0253-3219.2016.hjs.39.050403.
对液体闪烁探测器EJ339A中子与伽马辐射测量问题
采用理论模拟与实验分析方法
结合自主设计搭建的基于LabVIEW的数字化信号处理系统
分别完成
22
Na、
133
Ba、
137
Cs和
60
Co等4种不同能量的γ源等效电子能量测量与刻度。在此基础上
利用中子飞行时间测量原理
在不同时间窗下将锎(
252
Cf)源近似分化成若干个单能中子源
获得1.9-7.8MeV范围内中子在探测器中的光输出响应函数。结果表明
理论模拟与实验测量值在低能段比较吻合
而高能段存在约7.3%的误差。
Background:
2
The light output function is an elementary aspect for neutron spectrometry measured by an organic scintillator to unfold the neutron spectrum from the pulse height distribution.
Purpose:
2
This paper aims to investigate the properties of a boron-loaded liquid scintillator EJ339A
using photon sources and neutrons from a
252
Cf source.
Methods:
2
The light output was defined using Compton electron spectra. Pulse shape discrimination(PSD) and time of flight(TOF) were used to distinguish neutron and γ-rays. Combining theoretical modeling and experimental research
four different gamma sources are applied to achieve equivalent calibration of electronic energy
namely
22
Na
133
Ba
137
Cs
and
60
Co
respectively. Accordingly
based on TOF method
252
Cf
a spontaneous fission neutron source
is treated as several quasi-monoenergetic neutron sources under different time-windows.
Results:
2
The electron light output scale was calibrated by the measured detector response. Neutrons deposit energy in the detector and give a light output function with the neutron energy in the range of 1.9-7.8MeV.
Conclusion:
2
It shows that experimental data of light output function are in good agreement with simulation result in the low energy section
while discrepancies arise in the high energy section.
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