Rinecker Proton Therapy Center, Munich, Germany.
Department of Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München (LMU Munich), Munich, Germany.
Z Med Phys. 2019 May;29(2):162-172. doi: 10.1016/j.zemedi.2018.08.002. Epub 2018 Sep 22.
Proton beams used for radiotherapy have potential for superior sparing of normal tissue, although range uncertainties are among the main limiting factors in the accuracy of dose delivery. The aim of this study was to benchmark an N-vinylpyrrolidone based polymer gel to perform three-dimensional measurement of geometric proton beam characteristics and especially to test its suitability as a range probe in combination with an anthropomorphic phantom. For single proton pencil beams as well as for 3×3cm mono-energy layers depth dose profiles, lateral dose distribution at different depths and proton range were evaluated in simple cubic gel phantoms at different energies from 75 to 115MeV and different dose levels. In addition, a 90MeV mono-energetic beam was delivered to an anthropomorphic 3D printed head phantom, which was filled with gel. Subsequently, all phantoms underwent magnetic resonance imaging using an axial pixel size of 0.68-0.98mm and with slice thicknesses of 2 or 3mm to derive a 3-dimensional distribution of the T relaxation time, which correlates with radiation dose. Indices describing lateral dose distribution and proton range were compared against predictions from a treatment planning system (TPS, for cubic and head phantoms) and Monte Carlo simulations (MC, for the head phantom) after manual rigid co-registration with the T relaxation time datasets. For all pencil beams, the FWHM agreement with TPS was better than 1mm or 7%. For the mono-energetic layer, the agreement with TPS in this respect was even better than 0.3mm in each case. With respect to range, results from gel measurements differed no more than 0.9mm (1.6%) from values predicted by TPS. In case of the anthropomorphic phantom, deviations with respect to a nominal range of about 61mm as well as in FWHM were slightly higher, namely within 1.0mm and 1.1mm respectively. Average deviations between gel and TPS/MC were similar (-0.3mm±0.4mm/-0.2±0.5mm). In conclusion, polymer gel dosimetry was found to be a valuable tool to determine geometric proton beam properties three-dimensionally and with high spatial resolution in simple cubic as well as in a more complex anthropomorphic phantom. Post registration range errors of the order of 1mm could be achieved. The additional registration uncertainty (95%) was 1mm.
质子束用于放射治疗具有更好地保护正常组织的潜力,尽管射程不确定性是影响剂量传递准确性的主要限制因素之一。本研究的目的是基准一种基于 N-乙烯基吡咯烷酮的聚合物凝胶,以进行三维测量几何质子束特性,并特别测试其作为与人体模型相结合的射程探头的适用性。对于单质子铅笔束以及 3×3cm 单能量层深度剂量分布,在不同能量(75 至 115MeV)和不同剂量水平下,在简单立方凝胶模型中评估了不同深度和质子射程的横向剂量分布。此外,90MeV 单能束被传送到充满凝胶的人体模型 3D 打印头模型中。随后,所有模型都使用轴向像素大小为 0.68-0.98mm 和切片厚度为 2 或 3mm 的磁共振成像(MRI)进行成像,以得出与辐射剂量相关的 T 弛豫时间的三维分布。描述横向剂量分布和质子射程的指数与治疗计划系统(TPS,用于立方和头部模型)和蒙特卡罗模拟(MC,用于头部模型)的预测进行了比较,在手动刚性配准后与 T 弛豫时间数据集进行了比较。对于所有铅笔束,与 TPS 的 FWHM 一致性优于 1mm 或 7%。对于单能层,在这方面,与 TPS 的一致性甚至优于每个情况下的 0.3mm。关于射程,凝胶测量结果与 TPS 预测值的差异不超过 0.9mm(1.6%)。对于人体模型,与标称射程(约 61mm)以及 FWHM 的偏差略高,分别在 1.0mm 和 1.1mm 范围内。凝胶与 TPS/MC 之间的平均偏差相似(-0.3mm±0.4mm/-0.2±0.5mm)。总之,聚合物凝胶剂量测定被发现是一种有价值的工具,可以在简单立方和更复杂的人体模型中三维地确定几何质子束特性,并具有高空间分辨率。可以达到 1mm 左右的后注册射程误差。额外的注册不确定性(95%)为 1mm。