Calculation of the Effective Energy Release Centerʼs Position of Inorganic Scintillation Detectors for Calibration at Small “Source–Detector” Distances

IF 0.2 Q4 INSTRUMENTS & INSTRUMENTATION Devices and Methods of Measurements Pub Date : 2021-01-01 DOI:10.21122/2220-9506-2021-12-3-239-248
R. Lukashevich, G. Fokov
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Abstract

Inorganic scintillation detectors are widely used to measure of dose rate in the environment due to their high sensitivity to photon radiation. A distinctive feature when using such detectors is the need to take into account of the position of the effective energy release center. This peculiarity is actual when using measuring instruments with inorganic scintillation detectors as working standards during calibration at short “source–detector” distances in conditions of low-background shield or using a facility with protection from external gamma radiation background in the dose rate range from 0.03 to 0.3 μSv/h (μGy/h). The purpose of this work was to calculate the position of the effective energy release center of NaI(Tl) scintillation detectors and to take it into account when working at short “source–detector” distances.An original method of determining the position of the effective energy release center when irradiating the side and end surfaces of inorganic scintillation detector with parallel gamma radiation flux and point gamma radiation sources at small “source–detector” distances using Monte Carlo methods is proposed. The results of calculations of the position of the effective energy release center of NaI(Tl) based detectors of “popular” sizes for the cases of parallel gamma radiation flux and point sources of gamma radiation at small “source–detector” distances are presented. The functional dependences of the position of the effective energy release center of NaI(Tl) based detectors on the distance to the point gamma radiation sources and the energy of gamma radiation sources are presented.As a result of the study it was found that for scintillation NaI(Tl) detectors of medium size (for example, Ø25×40 mm or Ø40×40 mm) the point gamma radiation source located at a distance of 1 m or more, creates a radiation field which does not differ in characteristics from the radiation field created by a parallel flux of gamma radiation. It is shown that approaching the point gamma radiation source to the surface of scintillation detector leads to displacement of the position of the effective energy release center to the surface of the detector.
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小“源-探测器”距离下校准用无机闪烁探测器有效能量释放中心位置的计算
无机闪烁探测器因其对光子辐射的高灵敏度而被广泛应用于环境中剂量率的测量。使用这种探测器的一个显著特点是需要考虑到有效能量释放中心的位置。在低背景屏蔽条件下,在短“源-探测器”距离的校准中,或在剂量率范围为0.03至0.3 μSv/h (μGy/h)的外部伽马辐射背景下,使用带有无机闪烁探测器的测量仪器作为工作标准时,这种特性是实际存在的。本工作的目的是计算NaI(Tl)闪烁探测器的有效能量释放中心的位置,并在短“源-探测器”距离下工作时考虑它。提出了一种利用蒙特卡罗方法在小“源-探测器”距离处用平行伽玛辐射源和点伽玛辐射源照射无机闪烁探测器侧面和端面时确定有效能量释放中心位置的新颖方法。本文给出了在平行伽玛辐射通量和伽玛辐射源点距离较小的情况下,“流行”尺寸的NaI(Tl)基探测器有效能量释放中心位置的计算结果。给出了NaI(Tl)基探测器有效能量释放中心位置与点伽玛辐射源距离和伽玛辐射源能量的函数依赖关系。研究结果发现,对于中等尺寸的闪烁NaI(Tl)探测器(例如,Ø25×40 mm或Ø40×40 mm),位于1 m或以上距离的点伽玛辐射源产生的辐射场与平行伽玛辐射通量产生的辐射场在特征上没有区别。结果表明,伽玛辐射源点靠近闪烁探测器表面会导致有效能量释放中心的位置向探测器表面偏移。
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来源期刊
Devices and Methods of Measurements
Devices and Methods of Measurements INSTRUMENTS & INSTRUMENTATION-
自引率
25.00%
发文量
18
审稿时长
8 weeks
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