Department of Radiation Oncology, Massachusetts General Hospital and Harvard Medical School, Boston, MA 02114, USA.
Phys Med Biol. 2013 Jun 21;58(12):4137-56. doi: 10.1088/0031-9155/58/12/4137. Epub 2013 May 20.
Relative motion between a tumor and a scanning proton beam results in a degradation of the dose distribution (interplay effect). This study investigates the relationship between beam scanning parameters and the interplay effect, with the goal of finding parameters that minimize interplay. 4D Monte Carlo simulations of pencil beam scanning proton therapy treatments were performed using the 4DCT geometry of five lung cancer patients of varying tumor size (50.4-167.1 cc) and motion amplitude (2.9-30.1 mm). Treatments were planned assuming delivery in 35 × 2.5 Gy(RBE) fractions. The spot size, time to change the beam energy (τes), time required for magnet settling (τss), initial breathing phase, spot spacing, scanning direction, scanning speed, beam current and patient breathing period were varied for each of the five patients. Simulations were performed for a single fraction and an approximation of conventional fractionation. For the patients considered, the interplay effect could not be predicted using the superior-inferior motion amplitude alone. Larger spot sizes (σ ~ 9-16 mm) were less susceptible to interplay, giving an equivalent uniform dose (EUD) of 99.0 ± 4.4% (1 standard deviation) in a single fraction compared to 86.1 ± 13.1% for smaller spots (σ ~ 2-4 mm). The smaller spot sizes gave EUD values as low as 65.3% of the prescription dose in a single fraction. Reducing the spot spacing improved the target dose homogeneity. The initial breathing phase can have a significant effect on the interplay, particularly for shorter delivery times. No clear benefit was evident when scanning either parallel or perpendicular to the predominant axis of motion. Longer breathing periods decreased the EUD. In general, longer delivery times led to lower interplay effects. Conventional fractionation showed significant improvement in terms of interplay, giving a EUD of at least 84.7% and 100.0% of the prescription dose for the small and larger spot sizes respectively. The interplay effect is highly patient specific, depending on the motion amplitude, tumor location and the delivery parameters. Large degradations of the dose distribution in a single fraction were observed, but improved significantly using conventional fractionation.
肿瘤与扫描质子束之间的相对运动导致剂量分布的劣化(相互作用效应)。本研究调查了束扫描参数与相互作用效应之间的关系,目的是找到最小化相互作用效应的参数。使用五个不同肿瘤大小(50.4-167.1cc)和运动幅度(2.9-30.1mm)的肺癌患者的 4DCT 几何形状,对铅笔束扫描质子治疗进行了 4D Monte Carlo 模拟。假设以 35×2.5Gy(RBE)的分数进行治疗。对于五个患者中的每一个,都改变了光斑大小、改变束能量的时间(τes)、磁体稳定所需的时间(τss)、初始呼吸阶段、光斑间距、扫描方向、扫描速度、束电流和患者呼吸周期。对单次分割和常规分割进行了模拟。对于考虑的患者,仅使用上下运动幅度不能预测相互作用效应。较大的光斑尺寸(σ9-16mm)不易受相互作用影响,在单次分割中产生的均匀剂量(EUD)为 99.0±4.4%(1 个标准差),而较小光斑(σ2-4mm)的 EUD 为 86.1±13.1%。较小的光斑尺寸在单次分割中 EUD 值低至处方剂量的 65.3%。减小光斑间距可改善靶区剂量均匀性。初始呼吸阶段对相互作用有显著影响,特别是对于较短的治疗时间。平行或垂直于运动的主要轴扫描时,没有明显的好处。较长的呼吸周期会降低 EUD。一般来说,较长的治疗时间会导致相互作用效应降低。常规分割在相互作用方面有显著改善,小光斑和大光斑的 EUD 分别至少为处方剂量的 84.7%和 100.0%。相互作用效应高度取决于患者的个体情况,取决于运动幅度、肿瘤位置和治疗参数。在单次分割中观察到剂量分布的严重劣化,但使用常规分割可显著改善。