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1.四川理工学院 化学与环境工程学院 自贡 643000
2.中国工程物理研究院 核物理与化学研究所 绵阳 621900
3.西南科技大学 核废物与环境安全国防重点学科实验室 绵阳 621010
4.成都理工大学 地质灾害防治与地质环境保护国家重点实验室 成都 610059
[ "郑洪龙, 男, 1989年出生, 2016年毕业于西南科技大学, 现为博士研究生, 研究领域为核技术及应用", "ZHENG Honglong, male, born in1989, graduated from Southwest University of Science and Technology in 2016, doctoral student, focusing on nuclear technology and application" ]
庹先国, E-mail:myconnectionmail@126.com TUO Xianguo, E-mail:myconnectionmail@126.com
收稿日期:2016-11-14,
修回日期:2017-02-14,
纸质出版日期:2017-03-10
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郑洪龙, 庹先国, 石睿, 等. 蒙特卡罗模拟确定γ射线衰减系数函数及参数[J]. 核技术, 2017,40(3):030202
Honglong ZHENG, Xianguo TUO, Rui SHI, et al. Monte Carlo simulations of gamma ray linear attenuation coefficient function and determination of its parameters[J]. Nuclear techniques, 2017, 40(3): 030202
郑洪龙, 庹先国, 石睿, 等. 蒙特卡罗模拟确定γ射线衰减系数函数及参数[J]. 核技术, 2017,40(3):030202 DOI: 10.11889/j.0253-3219.2017.hjs.40.030202.
Honglong ZHENG, Xianguo TUO, Rui SHI, et al. Monte Carlo simulations of gamma ray linear attenuation coefficient function and determination of its parameters[J]. Nuclear techniques, 2017, 40(3): 030202 DOI: 10.11889/j.0253-3219.2017.hjs.40.030202.
在中低密度样品中,γ射线的线衰减系数主要由γ射线能量和样品密度决定,采用MCNP(Monte Carlo NParticle Transport Code)程序模拟计算了多种γ射线能量和多种样品密度条件下的线衰减系数,对线衰减系数模拟值进行多元非线性回归,确定了以γ射线能量和样品密度为因变量的线衰减系数函数及参数。实验测定了三种能量γ射线在6种不同密度样品中的线衰减系数值,并与模拟所得函数值进行比较分析。结果表明,所得函数值与实验值的相对误差均在7%以内,蒙特卡罗程序计算所得函数值与实验测量值较为吻合,所采用的函数模型准确验证了线衰减系数与γ射线能量、样品密度之间的关系特征。
Background
2
With low and intermediate level density sample
linear attenuation coefficient is mainly determined by gamma ray energy and material density.
Purpose
2
The aim is to determine the relationships and effect of gamma ray energy and material density to linear attenuation coefficient.
Methods
2
This work has constructed different samples with different densities from 0.3 g·cm
-3
to 3.0 g·cm
-3
by using Monte Carlo N Particle Transport Code (MCNP). Linear attenuation coefficients are obtained for gamma ray energies from 100 keV to 1 500 keV. Relationships and effect of gamma ray energy and material density to linear attenuation coefficient are determined by using a function model. Through experimental measurement of
137
Cs and
60
Co
linear attenuation coefficients are obtained for gamma ray energies 661.661 keV
1 173.238 keV
1 332.513 keV in different samples with densities from 1.0 g·cm
-3
to 2.7 g·cm
-3
.
Results
2
Relative deviations of linear attenuation coefficients between experimental and MCNP simulation results are less than 7%.
Conclusion
2
Simulation results are in good agreement with experimental measurement data. Linear attenuation coefficient function accurately reveals relationships and effect of gamma ray energy and material density to linear attenuation coefficient.
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