Department of Radiation Oncology and Particle Therapy Research Center, University Medical Center Groningen, University of Groningen, Groningen, The Netherlands.
Department of Radiation Science and Technology, Faculty of Applied Sciences, Delft University of Technology, Delft, The Netherlands.
Phys Med Biol. 2024 Nov 4;69(21). doi: 10.1088/1361-6560/ad897f.
The integration of proton beamlines with x-ray imaging/irradiation platforms has opened up possibilities for image-guided Bragg peak irradiations in small animals. Such irradiations allow selective targeting of normal tissue substructures and tumours. However, their small size and location pose challenges in designing experiments. This work presents a simulation framework useful for optimizing beamlines, imaging protocols, and design of animal experiments. The usage of the framework is demonstrated, mainly focusing on the imaging part.The fastCAT toolkit was modified with Monte Carlo (MC)-calculated primary and scatter data of a small animal imager for the simulation of micro-CT scans. The simulated CT of a mini-calibration phantom from fastCAT was validated against a full MC TOPAS CT simulation. A realistic beam model of a preclinical proton facility was obtained from beam transport simulations to create irradiation plans in matRad. Simulated CT images of a digital mouse phantom were generated using single-energy CT (SECT) and dual-energy CT (DECT) protocols and their accuracy in proton stopping power ratio (SPR) estimation and their impact on calculated proton dose distributions in a mouse were evaluated.The CT numbers from fastCAT agree within 11 HU with TOPAS except for materials at the centre of the phantom. Discrepancies for central inserts are caused by beam hardening issues. The root mean square deviation in the SPR for the best SECT (90 kV/Cu) and DECT (50 kV/Al-90 kV/Al) protocols are 3.7% and 1.0%, respectively. Dose distributions calculated for SECT and DECT datasets revealed range shifts <0.1 mm, gamma pass rates (3%/0.1 mm) greater than 99%, and no substantial dosimetric differences for all structures. The outcomes suggest that SECT is sufficient for proton treatment planning in animals.The framework is a useful tool for the development of an optimized experimental configuration without using animals and beam time.
质子束线与 X 射线成像/辐照平台的集成,为小动物的图像引导布拉格峰辐照开辟了可能性。这种辐照可以选择性地靶向正常组织亚结构和肿瘤。然而,它们的体积小和位置给实验设计带来了挑战。这项工作提出了一个有用的模拟框架,用于优化束线、成像协议和动物实验设计。主要聚焦于成像部分,展示了该框架的使用。
快速 CAT 工具包经过修改,使用了小动物成像器的蒙特卡罗(MC)计算的初级和散射数据,用于模拟微 CT 扫描。快速 CAT 模拟的微型校准体模的 CT 与完全 MC TOPAS CT 模拟进行了验证。通过束流传输模拟获得了临床前质子设施的真实束模型,以便在 matRad 中创建辐照计划。使用单能 CT(SECT)和双能 CT(DECT)协议生成数字老鼠体模的模拟 CT 图像,并评估其在质子阻止本领比(SPR)估计中的准确性及其对老鼠中计算的质子剂量分布的影响。
除了体模中心的材料外,快速 CAT 的 CT 数与 TOPAS 的吻合度在 11 HU 以内。中心插入物的差异是由于束硬化问题引起的。最佳 SECT(90 kV/Cu)和 DECT(50 kV/Al-90 kV/Al)协议的 SPR 中 RMS 偏差分别为 3.7%和 1.0%。SECT 和 DECT 数据集计算的剂量分布显示,射程偏移<0.1mm,伽马通过率(3%/0.1mm)大于 99%,所有结构的剂量学差异不大。结果表明,SECT 足以用于动物的质子治疗计划。
该框架是一种有用的工具,用于在不使用动物和束流时间的情况下开发优化的实验配置。