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使用卷积和叠加原理的剂量计算:发散X射线束中剂量分布核的方向

Dose calculations using convolution and superposition principles: the orientation of dose spread kernels in divergent x-ray beams.

作者信息

Sharpe M B, Battista J J

机构信息

Department of Medical Biophysics, University of Western Ontario, London, Canada.

出版信息

Med Phys. 1993 Nov-Dec;20(6):1685-94. doi: 10.1118/1.596955.

Abstract

The convolution/superposition method of dose calculation has the potential to become the preferred technique for radiotherapy treatment planning. When this approach is used for therapeutic x-ray beams, the dose spread kernels are usually aligned parallel to the central axis of the incident beam. While this reduces the computational burden, it is more rigorous to tilt the kernel axis to align it with the diverging beam rays that define the incident direction of primary photons. We have assessed the validity of the parallel kernel approximation by computing dose distributions using parallel and tilted kernels for monoenergetic photons of 2, 6, and 10 MeV; source-to-surface distances (SSDs) of 50, 80, and 100 cm; and for field sizes of 5 x 5, 15 x 15, and 30 x 30 cm2. Over most of the irradiated volume, the parallel kernel approximation yields results that differ from tilted kernel calculations by 3% or less for SSDs greater than 80 cm. Under extreme conditions of a short SSD, a large field size and high incident photon energy, the parallel kernel approximation results in discrepancies that may be clinically unacceptable. For 10-MeV photons, we have observed that the parallel kernel approximation can overestimate the dose by up to 4.4% of the maximum on the central axis for a field size of 30 x 30 cm2 applied with a SSD of 50 cm. Very localized dose underestimations of up to 27% of the maximum dose occurred in the penumbral region of a 30 x 30-cm2 field of 10-MeV photons applied with a SSD of 50 cm.

摘要

剂量计算的卷积/叠加方法有潜力成为放射治疗计划的首选技术。当这种方法用于治疗性X射线束时,剂量分布核通常与入射束的中心轴平行排列。虽然这减轻了计算负担,但将核轴倾斜使其与定义初级光子入射方向的发散束光线对齐会更严谨。我们通过使用平行核和倾斜核对2、6和10 MeV的单能光子、50、80和100 cm的源皮距(SSD)以及5×5、15×15和30×30 cm²的射野大小计算剂量分布,评估了平行核近似的有效性。在大多数受照体积内,对于SSD大于80 cm的情况,平行核近似产生的结果与倾斜核计算结果的差异在3%或更小。在SSD短、射野大且入射光子能量高的极端条件下,平行核近似会导致临床上可能无法接受的差异。对于10 MeV光子,我们观察到,对于50 cm的SSD应用30×30 cm²的射野,平行核近似在中心轴上的剂量高估可达最大值的4.4%。在50 cm的SSD应用10 MeV光子的30×30 cm²射野的半影区,出现了高达最大剂量27%的非常局部的剂量低估。

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