Department of Medical Physics, Memorial Sloan-Kettering Cancer Center, New York, NY 10065, USA.
J Appl Clin Med Phys. 2010 Jun 8;11(3):3182. doi: 10.1120/jacmp.v11i3.3182.
Respiration-induced tumor motion during intensity-modulated radiotherapy (IMRT) of non-small-cell lung cancer (NSCLC) could cause substantial differences between planned and delivered doses. While it has been shown that, for conventionally fractionated IMRT, motion effects average out over the course of many treatments, this might not be true for hypofractionated IMRT (IMHFRT). Numerical simulations were performed for nine NSCLC patients (11 tumors) to evaluate this problem. Dose distributions to the Clinical Target Volume (CTV) and Internal Target Volume (ITV) were retrospectively calculated using the previously-calculated leaf motion files but with the addition of typical periodic motion (i.e. amplitude 0.36-1.26cm, 3-8sec period). A typical IMHFRT prescription of 20Gy x 3 fractions was assumed. For the largest amplitude (1.26 cm), the average +/- standard deviation of the ratio of simulated to planned mean dose, minimum dose, D95 and V95 were 0.98+/-0.01, 0.88 +/- 0.09, 0.94 +/- 0.05 and 0.94 +/- 0.07 for the CTV, and 0.99 +/-0.01, 0.99 +/- 0.03, 0.98 +/- 0.02 and 1.00 +/- 0.01 for the ITV, respectively. There was minimal dependence on period or initial phase. For typical tumor geometries and respiratory amplitudes, changes in target coverage are minimal but can be significant for larger amplitudes, faster beam delivery, more highly-modulated fields, and smaller field margins.
在非小细胞肺癌(NSCLC)的调强放疗(IMRT)中,呼吸引起的肿瘤运动可能导致计划剂量和实际剂量之间存在显著差异。虽然已经表明,对于常规分割的调强放疗,运动效应会在多次治疗过程中平均化,但对于低分割调强放疗(IMHFRT)可能并非如此。针对这个问题,对 9 名 NSCLC 患者(11 个肿瘤)进行了数值模拟。使用之前计算的叶片运动文件,但增加了典型的周期性运动(即幅度为 0.36-1.26cm,周期为 3-8 秒),回顾性地计算了临床靶区(CTV)和内靶区(ITV)的剂量分布。假设典型的 IMHFRT 处方为 20Gy x 3 个分数。对于最大幅度(1.26cm),模拟与计划平均剂量、最小剂量、D95 和 V95 的比值的平均值 +/- 标准差分别为 0.98+/-0.01、0.88 +/- 0.09、0.94 +/- 0.05 和 0.94 +/- 0.07 用于 CTV,0.99 +/-0.01、0.99 +/- 0.03、0.98 +/- 0.02 和 1.00 +/- 0.01 用于 ITV。周期或初始相位的依赖性最小。对于典型的肿瘤几何形状和呼吸幅度,靶区覆盖的变化很小,但对于较大的幅度、更快的束流输送、调制程度更高的场和更小的场边缘,变化可能会显著。