诊断放射学中使用低剂量铯-137源校准MTS-N(LiF:Mg,Ti)芯片用于人员剂量测定

A. Omojola, M. Akpochafor, S. Adeneye, M. Aweda
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引用次数: 4

摘要

热发光剂量计(TLD)仍在许多应用中使用,如辐射防护、医疗剂量测定、环境研究和人员剂量测定,其总体目标是估计给定介质或材料内的辐射剂量。本研究的目的是确定同一条形码载玻片内热致发光(TL)元件的变异系数(CV),并为新购买的TL元件和新的RadPro TLD手动读取器和退火炉在组织中0.07 mm深度的剂量当量(Hp[0.07])和组织中10 mm深度的量量当量(Hp[10])下建立校准因子(CF)。退火的TL元素被带到二级标准剂量测定实验室(SSDL),使用已知剂量(0.2–2 mGy)的铯-137源进行辐照。使用RadPro Cube 400手动TLD读取器来确定相应的TL信号。确定了(Hp[10])和(Hp[0.07])条形码幻灯片中两个相同TL元素之间的CV,并绘制了剂量(mGy)与TL信号(库仑)的曲线图以确定元素CF。根据40个TL元素的原始数据,Hp(10)和Hp(0.07)的CV分别为14.6%和15.02%。对敏感TL元素的进一步选择使Hp(10)和Hp(0.07)的CV分别降低到3.73%和3.21%,在±10%的可接受限度内。Hp(10)和Hp(0.07)的计算剂量和实际剂量的最大百分比偏差分别为16.7%和14.3%。在对初始图进行调整后,CF为10−6的幂,Hp(10)和Hp(0.07)的决定系数(R2)分别为0.9998和0.9981。尽管在低剂量下观察到与原始数据的结果有很大的偏差。重新选择的“黄金芯片”的R2接近1,CV在推荐标准范围内。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Calibration of MTS-N (LiF: Mg, Ti) chips using cesium-137 source at low doses for personnel dosimetry in diagnostic radiology
Thermoluminescent dosimeter (TLD) is still in use for many applications such as radiation protection, medical dosimetry, environmental research, and personnel dosimetry, with the overall aim of estimating radiation dose within a given medium or material. The aim of this study was to determine the coefficient of variation (CV) for thermoluminescent (TL) element within the same bar-coded slide and to establish calibration factors (CFs) at dose equivalent of 0.07 mm depth in tissue (Hp [0.07]) and dose equivalent of 10 mm depth in tissue (Hp [10]) for newly purchased TL elements alongside a new RadPro TLD manual reader and annealing oven. Annealed TL elements were taken to a Secondary Standard Dosimetry Laboratory (SSDL) for irradiation using a cesium-137 source at known doses (0.2–2 mGy). A RadPro Cube 400 manual TLD Reader was used to determine corresponding TL signal. The CV between two identical TL element within a bar-coded slide for (Hp [10]) and (Hp [0.07]) was determined and a graph of dose (mGy) against TL signal (Coulomb) was plotted to determine the elements CF. CVs from the raw data for 40 TL elements for Hp (10) and Hp (0.07) were 14.6% and 15.02%, respectively. Further selection of sensitive TL elements reduced the CVs of Hp (10) and Hp (0.07) to 3.73% and 3.21%, respectively, which was seen to be within ±10% accepted limit. The maximum percentage deviation for the calculated and actual dose for Hp (10) and Hp (0.07) was 16.7% and 14.3%, respectively. The CFs were power of 10 − 6 and the Coefficient of determination (R2) for Hp (10) and Hp (0.07) was 0.9998 and 0.9981, respectively, after adjustments were made on the initial graphs. Although large deviations were observed at low doses from the results of the raw data. Re-selected “golden Chips” had R2 close to unity and CV was within recommended standards.
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