Paul Scherrer Institute (PSI), Center for Proton Therapy, 5232 Villigen PSI, Switzerland.
Phys Med Biol. 2018 Jul 11;63(14):145006. doi: 10.1088/1361-6560/aacd27.
Therapeutic pencil beams are typically scanned using one of the following three techniques: spot scanning, raster scanning or line scanning. While providing similar dose distributions to the target, these three techniques can differ significantly in their delivery time sequence. Thus, we can expect differences in effectiveness and time efficiency when trying to mitigate interplay effects using rescanning. At the Paul Scherrer Institute, we are able to irradiate treatment plans using either of the three delivery techniques. Hence, we can compare them directly with identical underlying machine parameters such as energy switching time or minimum/maximum beam current. For this purpose, we selected three different liver targets, optimized plans for spots, and converted them to equivalent raster and line scanning plans. In addition to the scanning technique, we varied the underlying motion curve, starting phase, prescription dose and rescanning strategy, which resulted in a total of 1584 4D dose calculations and 49 measurements. They indicate that rescanning becomes effective when achieving a high number of rescans for every dose element. Fixed minimum spot weights for spot and raster scanning machines often hamper this. By introducing adaptive scaling of the beam current within iso-energy layers for line scanning, we can flexibly lower the minimum weight whenever required and achieve higher rescanning capability. Averaged over all scenarios studied, volumetric rescanning is significantly more effective than layered provided the same number of rescans are applied. Fast lateral scanning contributes to the efficiency of rescanning. We observed that in any given time window, we can always perform more rescans using raster or line scanning compared to spot scanning irradiations. Thus, we conclude that line scanning represents a promising technique for rescanning by combining both effectiveness and efficiency.
点扫描、光栅扫描或线扫描。虽然这三种技术都能为靶区提供相似的剂量分布,但它们在剂量传递顺序上可能存在显著差异。因此,在尝试通过重扫描来减轻互作用效应时,我们可以预期在效果和时间效率上存在差异。在保罗谢勒研究所,我们可以使用这三种传输技术中的任何一种来放射治疗计划。因此,我们可以用相同的基本机器参数,如能量切换时间或最小/最大束流,直接对它们进行比较。为此,我们选择了三个不同的肝脏靶区,对点扫描进行了优化,并将其转换为等效的光栅和线扫描计划。除了扫描技术外,我们还改变了基础运动曲线、起始相位、处方剂量和重扫描策略,总共进行了 1584 次 4D 剂量计算和 49 次测量。结果表明,当每个剂量元素的重扫描次数达到较高水平时,重扫描才会变得有效。点扫描和光栅扫描机器的固定最小点权重往往会对此造成阻碍。通过在线扫描的等能层内引入束流自适应缩放,我们可以在需要时灵活降低最小权重,从而提高重扫描能力。在所有研究的场景中,体积重扫描比分层重扫描更有效,只要应用相同数量的重扫描即可。快速横向扫描有助于提高重扫描效率。我们观察到,在任何给定的时间窗口内,与点扫描照射相比,我们总是可以使用光栅或线扫描进行更多的重扫描。因此,我们得出结论,线扫描通过结合有效性和效率,代表了一种很有前途的重扫描技术。