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Comparison of RTP dose distributions in heterogeneous phantoms with the beam Monte Carlo simulation system

机译:光束蒙特卡罗模拟系统比较异形体中RTP剂量分布

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摘要

Therapeutic treatment plan evaluation is often based on examining the radiotherapy treatment planning (RTP) system dose distributions in the target and surrounding normal structures. To study the effects of tissue inhomogeneities on photon dose distributions, we compared FOCUS RTP system dose distributions from the measurement‐based Clarkson and model‐based MultiGrid Superposition (MGS) algorithms with those from the beam Monte Carlo code system in a set of heterogeneous phantoms. The phantom inhomogeneities mimic relevant clinical treatment sites, which include lung slab, lung‐bone slab, bone‐lung slab, mediastinum, and tumor geometries. The benchmark comparisons were performed in lung densities of 0.20 and 0.31g/cm3, and a bone density of 2.40g/cm3 for 5 × 5cm2 and 10 × 10cm2, 6 −  and 15‐MV photon beams. Benchmark comparison results show that the MGS model and beam doses match better than 3% or 3 mm, and the MGS model is more accurate than the Clarkson model in all phantoms. The MGS model, unlike the Clarkson model, predicts the build‐down and build‐up of dose near tissue interfaces and penumbra broadening in lung associated with high energy beams. The Clarkson model overestimates the dose in lung by a maximum of 10% compared to beam. Dose comparisons suggest turning‐off the effective path length inhomogeneity correction in the Clarkson model for lung treatments.PACS number(s): 87.53.–j, 87.53.Bn
机译:治疗计划的评估通常基于检查靶标和周围正常结构中的放射治疗计划(RTP)系统剂量分布。为了研究组织不均匀性对光子剂量分布的影响,我们在一组异质模型中比较了基于测量的Clarkson和基于模型的MultiGrid Superposition(MGS)算法的FOCUS RTP系统剂量分布与基于束蒙特卡罗编码系统的剂量分布。幻影异质性模仿了相关的临床治疗部位,包括肺厚片,肺骨厚片,骨肺厚片,纵隔和肿瘤的几何形状。在5×5cm 2 <的肺密度为0.20和0.31g / cm 3 和骨密度为2.40g / cm 3 的情况下进行基准比较。 / sup>和10×10cm 2 ,6−和15-MV光子束。基准比较结果表明,MGS模型和光束剂量的匹配度优于3%或3 mm,并且在所有体模中,MGS模型比Clarkson模型更准确。与克拉克森模型不同,MGS模型可预测与高能束有关的组织界面附近剂量的累积和累积以及肺半影变宽。与射线束相比,克拉克森模型高估了肺部剂量最多10%。剂量比较表明,应关闭Clarkson模型中用于肺部治疗的有效路径长度不均匀性校正。PACS数量:87.53.–j,87.53.Bn

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