Moreno-Pérez Juan Antonio, Marchena Álvaro, Araya Pablo, López-Peñalver Jesús J, de la Torre Juan Alejandro, Lallena Antonio M, Becerril Santiago, Anguiano Marta, Palma Alberto J, Carvajal Miguel A
Electronic and Chemical Sensing Solutions (ECsens), CITIC-UGR, Department of Electronics and Computer Technology, University of Granada, E-18014 Granada, Spain.
IFMIF-DONES España, Gran Vía de Colón, 48, E-18010 Granada, Spain.
Sensors (Basel). 2025 Mar 17;25(6):1862. doi: 10.3390/s25061862.
Various models of ionization and fission chambers for ionizing radiation detection, designed to operate under harsh conditions such as those found in fusion reactors or particle accelerators, have been experimentally characterized and numerically simulated. These models were calibrated using a photon beam in the X-ray spectrum. Irradiations were performed at the Biomedical Research Center of the University of Granada (CIBM) with a bipolar metal-ceramic X-ray tube operating at a voltage of 150 kV and a dose rate ranging from 0.05 to 2.28 Gy/min. All detectors under study featured identical external structures but varied in detection volume, anode configuration, and filling gas composition. To assess inter- and intra-model response variations, the tested models included 12 micro-ionization chambers (CRGR10/C5B/UG2), 3 micro-fission chambers (CFUR43/C5B-U5/UG2), 8 micro-fission chambers (CFUR43/C5B-U8/UG2), and 3 micro-fission chambers (CFUR44/C5B-U8/UG2), all manufactured by Photonis (Merignac, France). The experimental setup was considered suitable for the tests, as the leakage current was below 20 pA. The optimal operating voltage range was determined to be 130-150 V, and the photon sensitivities for the chambers were measured as 29.8 ± 0.3 pA/(Gy/h), 43.0 ± 0.8 pA/(Gy/h), 39.2 ± 0.3 pA/(Gy/h), and 96.0 ± 0.9 pA/(Gy/h), respectively. Monte Carlo numerical simulations revealed that the U layer in the fission chambers was primarily responsible for their higher sensitivities due to photoelectric photon absorption. Additionally, the simulations explained the observed differences in sensitivity based on the filling gas pressure. The detectors demonstrated linear responses to dose rates and high reproducibility, making them reliable tools for accurate determination of ionizing photon beams across a range of applications.
已对各种用于电离辐射检测的电离室和裂变室模型进行了实验表征和数值模拟,这些模型设计用于在聚变反应堆或粒子加速器等恶劣条件下运行。这些模型使用X射线光谱中的光子束进行了校准。在格拉纳达大学的生物医学研究中心(CIBM),使用双极金属陶瓷X射线管进行辐照,该X射线管的工作电压为150 kV,剂量率范围为0.05至2.28 Gy/min。所有研究的探测器都具有相同的外部结构,但检测体积、阳极配置和填充气体成分各不相同。为了评估模型间和模型内的响应变化,测试模型包括12个微电离室(CRGR10/C5B/UG2)、3个微裂变室(CFUR43/C5B-U5/UG2)、8个微裂变室(CFUR43/C5B-U8/UG2)和3个微裂变室(CFUR44/C5B-U8/UG2),均由Photonis公司(法国梅里尼亚克)制造。由于漏电流低于20 pA,实验装置被认为适合测试。确定最佳工作电压范围为130 - 150 V,各室的光子灵敏度分别测量为29.8 ± 0.3 pA/(Gy/h)、43.0 ± 0.8 pA/(Gy/h)、39.2 ± 0.3 pA/(Gy/h)和96.0 ± 0.9 pA/(Gy/h)。蒙特卡罗数值模拟表明,裂变室中的U层由于光电光子吸收,是其较高灵敏度的主要原因。此外,模拟还基于填充气体压力解释了观察到的灵敏度差异。这些探测器对剂量率表现出线性响应且具有高重现性,使其成为在一系列应用中准确测定电离光子束的可靠工具。