Tajiri Shinya, Tashiro Mutsumi, Mizukami Tomohiro, Tsukishima Chihiro, Torikoshi Masami, Kanai Tatsuaki
Department of Heavy Ion Beam Medical Physics and Biology, Gunma University Graduate School of Medicine, 3-39-22 Showa-Machi, Maebashi, Gunma 371-8511, Japan.
Mitsubishi Electric Corporation, 1-1-2, Wadasaki-cho, Hyogo-ku, Kobe 652-8555, Japan.
J Radiat Res. 2017 Nov 1;58(6):840-848. doi: 10.1093/jrr/rrx001.
Carbon-ion therapy by layer-stacking irradiation for static targets has been practised in clinical treatments. In order to apply this technique to a moving target, disturbances of carbon-ion dose distributions due to respiratory motion have been studied based on the measurement using a respiratory motion phantom, and the margin estimation given by the square root of the summation Internal margin2+Setup margin2 has been assessed. We assessed the volume in which the variation in the ratio of the dose for a target moving due to respiration relative to the dose for a static target was within 5%. The margins were insufficient for use with layer-stacking irradiation of a moving target, and an additional margin was required. The lateral movement of a target converts to the range variation, as the thickness of the range compensator changes with the movement of the target. Although the additional margin changes according to the shape of the ridge filter, dose uniformity of 5% can be achieved for a spherical target 93 mm in diameter when the upward range variation is limited to 5 mm and the additional margin of 2.5 mm is applied in case of our ridge filter. Dose uniformity in a clinical target largely depends on the shape of the mini-peak as well as on the bolus shape. We have shown the relationship between range variation and dose uniformity. In actual therapy, the upper limit of target movement should be considered by assessing the bolus shape.
临床治疗中已采用层叠照射法对静态靶区进行碳离子治疗。为了将该技术应用于移动靶区,基于使用呼吸运动体模的测量研究了呼吸运动引起的碳离子剂量分布扰动,并评估了由内部边缘²+设置边缘²之和的平方根给出的边缘估计值。我们评估了因呼吸而移动的靶区剂量与静态靶区剂量之比的变化在5%以内的体积。这些边缘对于移动靶区的层叠照射来说是不够的,还需要额外的边缘。由于射程补偿器的厚度随靶区移动而变化,靶区的横向移动会转化为射程变化。尽管额外边缘会根据脊形滤过器的形状而变化,但对于直径93mm的球形靶区,当向上射程变化限制在5mm且采用我们的脊形滤过器时应用2.5mm的额外边缘,可实现5%的剂量均匀性。临床靶区内的剂量均匀性在很大程度上取决于微峰的形状以及推注形状。我们已经展示了射程变化与剂量均匀性之间的关系。在实际治疗中,应通过评估推注形状来考虑靶区移动的上限。