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[使用针状电离室对不同深度微型体模的吸收剂量计算及散射因子测量的准确性]

[Accuracy of absorbed dose calculation and measurement of scatter factors with different depth of mini-phantoms using a pinpoint ionization chamber].

作者信息

Oita Masataka, Watanabe Yoshiharu, Fujita Katsuhisa, Furuya Teruo, Nankumo Junya, Oda Makoto

机构信息

Department of Radiology, Hokkaido University Hospital.

出版信息

Nihon Hoshasen Gijutsu Gakkai Zasshi. 2004 Nov;60(11):1604-10. doi: 10.6009/jjrt.kj00003326585.

DOI:10.6009/jjrt.kj00003326585
PMID:15568013
Abstract

The output factor of high-energy X-ray machines varies with collimation. According to Khan's theory, collimator and phantom scatter factors contribute to total scatter factor. For precise X-ray irradiation, the two factors need to be taken into consideration. To obtain proper factors, we made two original polystyrene cylindrical mini-phantoms. These phantoms are both 4 cm in diameter and have a pinpoint ion chamber placed at a depth of 5 cm and 10 cm, respectively. Using a 6 MV X-ray machine, collimator scatter factors were calculated for various field arrangements (i.e., field sizes ranging from 4 cm x 4 cm to 40 cm x 40 cm at isocenter). To determine if calculated values were appropriate, we measured point doses of 20 X-ray irradiation patterns using a Farmer-type ion chamber with a water equivalent phantom at depths of 5 cm and 10 cm, respectively. Two hundred MUs were irradiated to the above-mentioned depths for each field. Based on the measured doses, variations were obtained for four calculation methods. Accounting for 1) secondary collimator (jaw) setting, 2) blocked field (multi-leaf collimator) setting, 3) Khan's theory using a 5 cm mini-phantom, and 4) Khan's theory using a 10 cm mini-phantom. Dose variations in each method of calculation were as follows: 1) +0.3 to +10.2% (mean, +2.0 to +3.2%) , 2) -2.3 to 0.0% (mean, -0.8 to -0.6%), 3) 0.0 to +1.5% (mean, +0.1 to +0.3%), 4) 0.0 to +1.4% (mean, -0.1 to +0.1%).

摘要

高能X射线机的输出因子随准直而变化。根据汗氏理论,准直器和体模散射因子构成总散射因子。对于精确的X射线照射,需要考虑这两个因素。为了获得合适的因子,我们制作了两个原始的聚苯乙烯圆柱形小型体模。这些体模的直径均为4 cm,分别在深度5 cm和10 cm处放置了一个针点电离室。使用一台6 MV X射线机,针对各种射野布置(即等中心处射野尺寸范围为4 cm×4 cm至40 cm×40 cm)计算准直器散射因子。为了确定计算值是否合适,我们分别使用一个水等效体模的 Farmer 型电离室,测量了20种X射线照射模式在深度5 cm和10 cm处的点剂量。对每个射野在上述深度照射200 MU。根据测量剂量,获得了四种计算方法的变化情况。分别考虑1)二级准直器(光阑)设置,2)遮挡射野(多叶准直器)设置,3)使用5 cm小型体模的汗氏理论,以及4)使用10 cm小型体模的汗氏理论。每种计算方法的剂量变化如下:1)+0.3%至+10.2%(平均值,+2.0%至+3.2%),2)-2.3%至0.0%(平均值,-0.8%至-0.6%),3)0.0%至+1.5%(平均值,+0.1%至+0.3%),4)0.0%至+1.4%(平均值,-0.1%至+0.1%)。

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