OncoRay-National Center for Radiation Research in Oncology, Medical Faculty Carl Gustav Carus, TU Dresden, Fetscherstraße 74, PF 41, D-01307 Dresden, Germany.
Phys Med Biol. 2013 Feb 7;58(3):513-33. doi: 10.1088/0031-9155/58/3/513. Epub 2013 Jan 10.
Particle therapy positron emission tomography (PT-PET) allows for an in vivo and in situ verification of applied dose distributions in ion beam therapy. Since the dose distribution cannot be extracted directly from the β(+)-activity distribution gained from the PET scan the validation is done by means of a comparison between the reconstructed β(+)-activity distributions from a PT-PET measurement and from a PT-PET simulation. Thus, the simulation software for generating PET data predicted from the treatment planning is an essential part of the dose verification routine. For the dose monitoring of intra-fractionally moving target volumes the PET data simulation needs to be upgraded by using time resolved (4D) algorithms to account correctly for the motion dependent displacement of the positron emitters. Moreover, it has to consider the time dependent relative movement between target volume and scanned beam to simulate the accurate positron emitter distribution generated during irradiation. Such a simulation program is presented which properly proceeds with motion compensated dose delivery by scanned ion beams to intra-fractionally moving targets. By means of a preclinical phantom study it is demonstrated that even the sophisticated motion-mitigated beam delivery technique of range compensated target tracking can be handled correctly by this simulation code. The new program is widely based on the 3D PT-PET simulation program which had been developed at the Helmholtz-Zentrum Dresden-Rossendorf, Germany (HZDR) for application within a pilot project to simulate in-beam PET data for about 440 patients with static tumor entities irradiated at the former treatment facility of the GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany (GSI). A simulation example for a phantom geometry irradiated with a tracked (12)C-ion beam is presented for demonstrating the proper functionality of the program.
粒子治疗正电子发射断层扫描(PT-PET)允许在体内和原位验证离子束治疗中应用的剂量分布。由于无法直接从 PET 扫描获得的β(+)活性分布中提取剂量分布,因此验证是通过比较从 PT-PET 测量和 PT-PET 模拟中重建的β(+)活性分布来完成的。因此,用于生成根据治疗计划预测的 PET 数据的仿真软件是剂量验证程序的重要组成部分。对于分次内移动靶区的剂量监测,需要使用时间分辨(4D)算法升级 PET 数据模拟,以正确考虑正电子发射体的运动相关位移。此外,它必须考虑靶区和扫描束之间的时变相对运动,以模拟在照射过程中生成的准确正电子发射体分布。本文提出了一种适用于分次内移动目标的运动补偿扫描离子束剂量监测的模拟程序。通过临床前体模研究表明,即使是具有复杂运动缓解功能的束流传输技术,如射程补偿的靶区跟踪,也可以由该模拟代码正确处理。新程序广泛基于德国德累斯顿-罗斯多夫亥姆霍兹中心(HZDR)开发的 3D PT-PET 模拟程序,该程序用于模拟在德国达姆施塔特 GSI 重离子研究中心(GSI)的前治疗设施中对 440 例静态肿瘤实体进行照射的体内 PET 数据。为了演示程序的正确功能,给出了一个用跟踪(12)C 离子束照射的体模几何结构的模拟示例。