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A novel dose rate optimization method to maximize ultra-high dose rate coverage of critical organs-at-risk without compromising dosimetry metrics in proton pencil beam scanning FLASH radiotherapy

束流扫描 剂量学 剂量率 闪光灯(摄影) 核医学 铅笔(光学) 质子疗法 医学物理学 放射治疗 材料科学 医学 光学 物理 放射科
作者
Xingyi Zhao,Sheng Huang,Haibo Lin,J. Isabelle Choi,Kun Zhu,Charles B. Simone,Xueqing Yan,Minglei Kang
出处
期刊:International Journal of Radiation Oncology Biology Physics [Elsevier]
标识
DOI:10.1016/j.ijrobp.2024.06.002
摘要

Purpose To investigate a dose rate optimization framework based on the spot scanning patterns to improve ultra-high dose rate coverage of critical organs-at-risk (OARs) for proton PBS FLASH radiotherapy, and to present implementation of a genetic algorithm (GA) method for spot sequence optimization to achieve PBS FLASH dose rate optimization under relatively low nozzle beam currents. Materials and Methods Firstly, a multi-field FLASH plan was developed to meet all the dosimetric goals and optimal FLASH dose rate coverage by considering the deliverable minimum MU (MMU) constraint. Then, a GA method was implemented into the in-house treatment platform to maximize the dose rate by exploring the best spot delivery sequence. A phantom study was performed to evaluate the effectiveness of the dose rate optimization. Then, 10 consecutive plans for lung cancer patients previously treated using PBS intensity-modulated proton therapy (IMPT) were optimized using 45 GyRBE in 3 fractions both transmission and Bragg peak FLASH-RT for further validation. The spot delivery sequence of each treatment field was optimized using this GA. The ultra-high dose rate volume histogram (DRVH) and dose rate coverage V40GyRBE/s were investigated to assess the efficacy of dose rate optimization quantitatively. Results Using a relatively low MU/spot of 150, corresponding to nozzle beam current of 65 nA, the FLASH dose rate ratio V40GyRBE/s of the OAR contour of the core was increased from 0 to ∼60% in the phantom study. In the lung cancer patients, the ultra-high dose rate coverage V40GyRBE/s were improved from 15.2%, 15.5%, 17.6%, and 16.0% before the delivery sequence optimization, to 31.8%, 43.5%, 47.6%, and 30.5% after delivery sequence optimization, in the lungs-GTV, spinal cord, esophagus, and heart (p-values all<0.001). When beam current increased to 130 nA, V40GyRBE/s was improved from 45.1%, 47.1%, 51.2%, and 51.4%, to 65.3%, 83.5%, 88.1%, and 69.4% (p-values<0.05). The averaged V40GyRBE/s for the target and OARs was increased from 12.9% to 41.6%, and 46.3% to 77.5% for 65 and 130 nA, respectively, showing significant improvements based on a clinical proton system. After optimizing the dose rate for the Bragg peak FLASH technique with a beam current of 340 nA, the V40GyRBE/s for the lung-GTV, spinal cord, esophagus, and heart were increased by 8.9%, 15.8%, 22%, and 20.8%, respectively. Conclusion An optimal plan quality can be maintained as the spot delivery sequence optimization is a separate independent process after the plan optimization. Both the phantom and patient results demonstrated that novel spot delivery sequence optimization can effectively improve the ultra-high dose rate coverage for critical OARs, which can potentially be applied in clinical practice for better OARs sparing efficacy.
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