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使用弗里克系统测定192Ir高剂量率近距离放射治疗源在参考点d(r0, θ0)处水中的吸收剂量。

Determination of absorbed dose in water at the reference point d(r0, theta0) for an 192Ir HDR brachytherapy source using a Fricke system.

作者信息

Austerlitz C, Mota H C, Sempau J, Benhabib S M, Campos D, Allison R, DeAlmeida C E, Zhu D, Sibata C H

机构信息

Department of Radiation Oncology, East Carolina University, Greenville, North Carolina 27834, USA.

出版信息

Med Phys. 2008 Dec;35(12):5360-5. doi: 10.1118/1.2996178.

Abstract

A ring-shaped Fricke device was developed to measure the absolute dose on the transverse bisector of a 192Ir high dose rate (HDR) source at 1 cm from its center in water, D(r0, theta0). It consists of a polymethylmethacrylate (PMMA) rod (axial axis) with a cylindrical cavity at its center to insert the 192Ir radioactive source. A ring cavity around the source with 1.5 mm thickness and 5 mm height is centered at 1 cm from the central axis of the source. This ring cavity is etched in a disk shaped base with 2.65 cm diameter and 0.90 cm thickness. The cavity has a wall around it 0.25 cm thick. This ring is filled with Fricke solution, sealed, and the whole assembly is immersed in water during irradiations. The device takes advantage of the cylindrical geometry to measure D(r0, theta0). Irradiations were performed with a Nucletron microselectron HDR unit loaded with an 192Ir Alpha Omega radioactive source. A Spectronic 1001 spectrophotometer was used to measure the optical absorbance using a 1 mL quartz cuvette with 1.00 cm light pathlength. The PENELOPE Monte Carlo code (MC) was utilized to simulate the Fricke device and the 192Ir Alpha Omega source in detail to calculate the perturbation introduced by the PMMA material. A NIST traceable calibrated well type ionization chamber was used to determine the air-kerma strength, and a published dose-rate constant was used to determine the dose rate at the reference point. The time to deliver 30.00 Gy to the reference point was calculated. This absorbed dose was then compared to the absorbed dose measured by the Fricke solution. Based on MC simulation, the PMMA of the Fricke device increases the D(r0, theta0) by 2.0%. Applying the corresponding correction factor, the D(r0, theta0) value assessed with the Fricke device agrees within 2.0% with the expected value with a total combined uncertainty of 3.43% (k=1). The Fricke device provides a promising method towards calibration of brachytherapy radiation sources in terms of D(r0, theta0) and audit HDR source calibrations.

摘要

研发了一种环形弗里克剂量仪,用于测量在水中距离192铱高剂量率(HDR)源中心1厘米处的横向平分线处的绝对剂量D(r0, θ0)。它由一根聚甲基丙烯酸甲酯(PMMA)棒(轴)组成,其中心有一个圆柱形腔,用于插入192铱放射源。围绕源的环形腔厚度为1.5毫米,高度为5毫米,以距离源中心轴1厘米为中心。这个环形腔蚀刻在一个直径2.65厘米、厚度0.90厘米的圆盘形基座中。腔周围有一个0.25厘米厚的壁。这个环充满弗里克溶液,密封,并且在照射期间整个组件浸入水中。该剂量仪利用圆柱几何形状来测量D(r0, θ0)。使用装有192铱阿尔法欧米伽放射源的Nucletron微选择器HDR装置进行照射。使用Spectronic 1001分光光度计,使用光程长度为1.00厘米的1毫升石英比色皿测量吸光度。利用PENELOPE蒙特卡罗代码(MC)详细模拟弗里克剂量仪和192铱阿尔法欧米伽源,以计算PMMA材料引入的扰动。使用可溯源至美国国家标准与技术研究院(NIST)校准的井型电离室确定空气比释动能强度,并使用已发表的剂量率常数确定参考点处的剂量率。计算了向参考点输送30.00戈瑞所需的时间。然后将该吸收剂量与弗里克溶液测量的吸收剂量进行比较。基于MC模拟,弗里克剂量仪的PMMA使D(r0, θ0)增加了2.0%。应用相应的校正因子,用弗里克剂量仪评估的D(r0, θ0)值与预期值在2.0%以内一致,总合成不确定度为3.43%(k = 1)。就D(r0, θ0)而言,弗里克剂量仪为近距离放射治疗辐射源的校准以及审核HDR源校准提供了一种有前景的方法。

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