Calibration system correction factor for measuring the reference air kerma rate (RAKR) applied to high dose rate 192Ir sources (HDR)

克尔玛 校准 物理 电离室 电离 平方反比定律 计算物理学 近距离放射治疗 核医学 光学 剂量学 放射治疗 医学 离子 经典力学 量子力学 万有引力 内科学
作者
Douglas Batista da Silva,Ademir Xavier da Silva,Carlos Frederico Estrada Alves,Luís Alexandre Gonçalves Magalhães
出处
期刊:Biomedical Physics & Engineering Express [IOP Publishing]
卷期号:10 (3): 035034-035034
标识
DOI:10.1088/2057-1976/ad35cd
摘要

Abstract The aim of this study was to use computer simulation to analyze the impact of the aluminum fixing support on the Reference Air Kerma (RAK), a physical quantity obtained in a calibration system that was experimentally developed in the Laboratory of Radiological Sciences of the University of the State of Rio de Janeiro (LCR-UERJ). Correction factors due to scattered radiation and the geometry of the 192 Ir sources were also sought to be determined. The computational simulation was validated by comparing some parameters of the experimental results with the computational results. These parameters were: verification of the inverse square law of distance, determination of (RAKR), analysis of the source spectrum with and without encapsulation, and the sensitivity curve of the Sourcecheck 4PI ionization chamber response, as a function of the distance from the source along the axial axis, using the microSelectron-v2 (mSv2) and GammaMedplus (GMp) sources. Kerma was determined by activity in the Reference air, with calculated values of 1.725 × 10 −3 U. Bq −1 and 1.710 × 10 −3 U. Bq −1 for the ionization chamber NE 2571 and TN 30001, respectively. The expanded uncertainty for these values was 0.932% and 0.919%, respectively, for a coverage factor (k = 2). The correction factor due to the influence of the aluminum fixing support for measurements at 1 cm and 10 cm from the source was 0.978 and 0.969, respectively. The geometric correction factor of the sources was k sg = 1.005 with an expanded uncertainty of 0.7% for a coverage factor (k = 2). This value has a difference of approximately 0.2% compared to the experimental values.
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