Chua Clifford Ghee Ann, Furutani Keith M, Lee Kang Hao, Lew Kah Seng, Koh Calvin Wei Yang, Wibawa Andrew, Master Zubin, Lew Wen Siang, Lee James Cheow Lei, Beltran Chris J, Park Sung Yong, Tan Hong Qi
Division of Radiation Oncology, National Cancer Centre Singapore, Singapore, Singapore.
Division of Physics and Applied Physics, School of Physical and Mathematical Science, Nanyang Technological University, Singapore, Singapore.
Phys Med Biol. 2025 Jul 7;70(14). doi: 10.1088/1361-6560/ade92a.
To comprehensively characterize the temporal characteristics of dose-driven continuous scanning (DDCS) proton therapy system including the rise time to nominal beam current (trise), minimum time between break spot (tb), beam current fluctuation and the flap dose.Measurements were performed on a Hitachi proton therapy synchrotron. The beam current fluctuation was measured using a 20 kHz 2D strip ionization chamber (CROSSmini) with a fixed point irradiation without break points (BPs).trise,tband flap dose were quantified using an oscilloscope connected to the radiofrequency knockout (RFK), high-speed switching magnet (HSST), and dose monitor signals. These measurements were performed with BPs.trisewas measured and compared using both the analytical log file based and direct measurement approaches. The measurements were performed across three energies (70.2, 150.2 and 228.7 MeV), three beam currents (8, 14 and 20 MU s) and five different spot MUs (6, 10, 20, 30 and 40 MU).The instantaneous beam current measured by CROSSmini showed fluctuations of up to 65%. After applying a 1.0 ms moving average, the beam current coincides with the log file recorded beam current, thereby validating the latter data. The time delay between RFK off and HSST on was (0.08 ± 0.01) ms and minimal flap dose was recorded with an average of 4MU. The minimum time between break spots was measured to be (1.67 ± 0.04) ms. The analytical log file-based and direct measurement oftrisewere correlated with a Pearson correlation coefficient of 0.86. Thetrisemeasurement across the entire spills showed a dependence on beam current where 8 MU shad a notably highertrisethan 14 and 20 MU s.This is the first comprehensive study to characterize the temporal properties of a DDCS proton therapy system. The methodology introduced in this work would help in the proton DDCS commissioning efforts in other centers.
为全面表征剂量驱动连续扫描(DDCS)质子治疗系统的时间特性,包括达到标称束流的上升时间(trise)、断点之间的最短时间(tb)、束流波动和瓣形剂量。在日立质子治疗同步加速器上进行了测量。使用20 kHz二维条形电离室(CROSSmini)在无断点(BP)的定点照射下测量束流波动。trise、tb和瓣形剂量通过连接到射频敲出(RFK)、高速开关磁铁(HSST)和剂量监测信号的示波器进行量化。这些测量是在有BP的情况下进行的。trise使用基于分析日志文件和直接测量的方法进行测量和比较。测量在三种能量(70.2、150.2和228.7 MeV)、三种束流(8、14和20 MU/s)以及五种不同的光斑MU(6、10、20、30和40 MU)下进行。CROSSmini测量的瞬时束流显示波动高达65%。应用1.0 ms移动平均值后,束流与日志文件记录的束流一致,从而验证了后者的数据。RFK关闭和HSST开启之间的时间延迟为(0.08±0.01)ms,记录的最小瓣形剂量平均为4 MU。断点之间的最短时间测量为(1.67±0.04)ms。基于分析日志文件的trise测量和直接测量的trise之间的Pearson相关系数为0.86。整个脉冲期间的trise测量显示出对束流的依赖性,其中8 MU/s的trise明显高于14和20 MU/s。这是首次全面表征DDCS质子治疗系统时间特性的研究。本工作中介绍的方法将有助于其他中心的质子DDCS调试工作。