Department of Physics, ETH Zurich, 8092 Zurich, Switzerland. Proton Therapy Center, Paul Scherrer Institute, 5232 Villigen PSI, Switzerland.
Phys Med Biol. 2013 Nov 21;58(22):7905-20. doi: 10.1088/0031-9155/58/22/7905. Epub 2013 Oct 29.
In recent years, particle therapy has become a widely accepted form of cancer treatment and technological advances in beam delivery technology (i.e. pencil beam scanning (PBS)) have enabled the application of highly conformal dose distributions to static targets. Current research focuses on the possibilities for the treatment of mobile targets with these techniques. Of different motion mitigation methods being investigated, rescanning is perhaps the easiest to apply clinically. In general however, different PBS delivery systems exhibit a different temporal parameter space between delivery and target motions, due to the system specific beam position adjustment times (BPATs). Depending on these BPATs, dosimetric effects appearing during irradiation of moving targets vary significantly. In this work, volumetric and layered rescanning were compared for four different scenarios--a combination of fast and slow BPATs laterally (4 ms and 10 ms) and in depth (80 ms and 1 s); and nine different treatment plan arrangements for two clinical liver cases. 4D dose calculations were performed assuming regular, sinusoidal rigid motion as a worst-case motion scenario to model interplay effects. Calculations were sampled over three different starting phases resulting in a total of 432 dose distributions. It was found that layered rescanning is the method of choice for slow scanning systems, both in terms of dose homogeneity (D5-95 values are lower by up to 16% with layered rescanning) and in the estimated treatment delivery times (reduction of up to 300 s with layered rescanning). Analysis of dose homogeneity showed that layered rescanning leads to a smoother decrease in dose inhomogeneity as a function of the number of rescans than volumetric rescanning, which shows larger fluctuations. However, layered rescanning appears to be more sensitive to the starting phase. When analyzing the performance of both approaches and different scanning speeds as a function of delivery time, layered rescanning appears to be the only viable approach for slow energy changing systems, even approaching the performance of fast energy changing systems, as long as lateral scanning speeds are kept high. Similar results were found for multiple field plans and when analyzing different field directions.
近年来,粒子治疗已成为一种广泛接受的癌症治疗形式,束流输送技术(即铅笔束扫描(PBS))的技术进步使静态靶区能够应用高适形剂量分布。目前的研究重点是利用这些技术治疗移动靶区的可能性。在正在研究的不同运动缓解方法中,重新扫描可能是最容易在临床上应用的方法。然而,不同的 PBS 输送系统由于系统特定的束位置调整时间(BPAT),在输送和目标运动之间表现出不同的时间参数空间。根据这些 BPAT,在照射移动靶区时出现的剂量学效应差异很大。在这项工作中,比较了四种不同情况的体积和分层重新扫描:横向快速和慢速 BPAT(4 ms 和 10 ms)以及深度快速和慢速 BPAT(80 ms 和 1 s)的组合;以及两个临床肝脏病例的九种不同的治疗计划安排。假设规则、正弦刚性运动为最坏情况运动场景进行 4D 剂量计算,以模拟相互作用效应。在三个不同的起始相位上进行计算,总共得到 432 个剂量分布。结果发现,对于慢速扫描系统,分层重新扫描是首选方法,无论是在剂量均匀性方面(分层重新扫描的 D5-95 值低 16%),还是在估计的治疗输送时间方面(分层重新扫描减少 300 s)。剂量均匀性分析表明,与体积重新扫描相比,分层重新扫描导致剂量不均匀性随重新扫描次数的平滑降低,而体积重新扫描则显示出较大的波动。然而,分层重新扫描似乎对起始相位更敏感。当分析两种方法和不同扫描速度作为输送时间的函数的性能时,分层重新扫描似乎是慢速能量变化系统唯一可行的方法,即使接近快速能量变化系统的性能,只要保持高横向扫描速度。当分析多个射野计划和不同射野方向时,也得到了类似的结果。