测定了能量为14.1 MeV的中子在碳核上非弹性散射形成的能量为4.43 MeV的g量子的NaI探测器的响应函数

Q4 Physics and Astronomy
S. Dabylova, Yu. N. Kopach, S. Sakhiyev, D. Grozdanov, N. Fedorov
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引用次数: 0

摘要

这项工作致力于确定探测器NaI(Tl)对能量为4.43MeV的g量子的响应函数,该量子是在能量为14.1MeV的中子在核12C上的非弹性散射过程中形成的。在伽马光谱法中,记录输出脉冲,其振幅与入射光子在检测介质中损失的能量成比例。辐射探测的主要任务之一是从探测器输出端测量的信号中恢复辐射特性。为此,有必要首先了解探测器作为辐射信号转换器的一般特性。探测器的主要特征是其响应函数,该函数可以定义为具有给定性质的粒子在探测器中产生特定信号的概率,该信号将被设备记录。本文介绍了基于NaI(Tl)晶体的闪烁探测器对非弹性快中子散射伽马辐射的响应函数建模结果,以研究其形成机制。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Determination of the response function of the NaI detector for g-quanta with an energy of 4.43 MeV, formed during inelastic scattering of neutrons with an energy of 14.1 MeV on carbon nuclei
The work is devoted to determining the response function of the detector NaI(Tl) for g -quanta with energy of 4.43 MeV, formed during inelastic scattering of neutrons with energy of 14.1 MeV on the nuclei 12C. In gamma spectrometry, output pulses are recorded, the amplitudes of which are proportional to the energy lost in the detection medium by incident photons. One of the main tasks of radiation detection is to restore radiation characteristics from signals measured at the outputs of detectors. For this, it is necessary to know, first of all, the general characteristics of detectors as converters of radiation into signals. The main characteristic of the detector is its response function, which can be defined as the probability that a particle with given properties generates a certain signal in the detector that will be registered by the device. The article presents the results of modeling the response function of a scintillation detector based on a NaI(Tl) crystal for gamma radiation from inelastic fast neutron scattering in order to study the mechanism of its formation.
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来源期刊
Eurasian Journal of Physics and Functional Materials
Eurasian Journal of Physics and Functional Materials Materials Science-Materials Science (miscellaneous)
CiteScore
1.10
自引率
0.00%
发文量
23
审稿时长
5 weeks
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