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Comparing calibration methods of electron beams using plane-parallel chambers with absorbed-dose to water based protocols.

机译:使用具有吸收剂量的水平面协议比较平面平行腔室的电子束校准方法。

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摘要

Recent absorbed-dose-based protocols allow for two methods of calibrating electron beams using plane-parallel chambers, one using the N(Co)D,w for a plane-parallel chamber, and the other relying on cross-calibration of the plane-parallel chamber in a high-energy electron beam against a cylindrical chamber which has an N(Co)D,w factor. The second method is recommended as it avoids problems associated with the Pwall correction factors at 60Co for plane-parallel chambers which are used in the determination of the beam quality conversion factors. In this article we investigate the consistency of these two methods for the PTW Roos, Scanditronics NACP02, and PTW Markus chambers. We processed our data using both the AAPM TG-51 and the IAEA TRS-398 protocols. Wall correction factors in 60Co beams and absorbed-dose beam quality conversion factors for 20 MeV electrons were derived for these chambers by cross-calibration against a cylindrical ionization chamber. Systematic differences of up to 1.6% were found between our values of Pwall and those from the Monte Carlo calculations underlying AAPM TG-51, and up to 0.6% when comparing with the IAEA TRS-398 protocol. The differences in Pwall translate directly into differences in the beam quality conversion factors in the respective protocols. The relatively large spread in the experimental data of Pwall, and consequently the absorbed-dose beam quality conversion factor, confirms the importance of the cross-calibration technique when using plane-parallel chambers for calibrating clinical electron beams. We confirmed that for well-guarded plane-parallel chambers, the fluence perturbation correction factor at d(max) is not significantly different from the value at d(ref). For the PTW Markus chamber the variation in the latter factor is consistent with published fits relating it to average energy at depth.
机译:最近的基于吸收剂量的协议允许使用平面平行腔室校准电子束的两种方法,一种使用平面平行腔室的N(Co)D,w,另一种依赖于平面平行腔室的交叉校准。在高能电子束中的平行腔室对着具有N(Co)D,w因子的圆柱形腔室。建议使用第二种方法,因为它避免了与用于确定光束质量转换因子的平面平行腔室在60Co时的Pwall校正因子有关的问题。在本文中,我们研究了PTW Roos,Scanditronics NACP02和PTW Markus腔室这两种方法的一致性。我们使用AAPM TG-51和IAEA TRS-398协议处理了数据。通过对圆柱电离室进行交叉校准,得出了这些室的60Co束中的壁校正因子和20 MeV电子的吸收剂量束质量转换因子。我们的Pwall值与AAPM TG-51的蒙特卡洛计算值之间的系统差异高达1.6%,与IAEA TRS-398协议相比,系统差异高达0.6%。 Pwall中的差异直接转化为相应协议中光束质量转换因子的差异。 Pwall实验数据中的相对较大的分布,以及因此的吸收剂量束质量转换因子,证实了在使用平面平行腔室校准临床电子束时交叉校准技术的重要性。我们确认,对于防护良好的平面平行腔室,d(max)处的注量扰动校正因子与d(ref)处的值无明显差异。对于PTW Markus室,后一个因子的变化与已公布的拟合将其与深度平均能量相关联。

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