Oancea Cristina, Sykorova Katerina, Jakubek Jan, Pivec Jiri, Riemer Felix, Worm Steven, Bourgouin Alexandra
ADVACAM, U Pergamenky 12, 170 00 Prague 7, Czech Republic.
ADVACAM, U Pergamenky 12, 170 00 Prague 7, Czech Republic.
Phys Med. 2025 Jan;129:104872. doi: 10.1016/j.ejmp.2024.104872. Epub 2024 Dec 11.
FLASH radiotherapy necessitates the development of advanced Quality Assurance methods and detectors for accurate monitoring of the radiation field. This study introduces enhanced time-resolution detection systems and methods used to measure the delivered number of pulses, investigate temporal structure of individual pulses and dose-per-pulse (DPP) based on secondary radiation particles produced in the experimental room.
A 20 MeV electron beam generated from a linear accelerator (LINAC) was delivered to a water phantom. Ultra-high dose-per-pulse electron beams were used with a dose-per-pulse ranging from ̴ 1 Gy to over 7 Gy. The pulse lengths ranged from 1.18 µs to 2.88 µs at a pulse rate frequency of 5 Hz. A semiconductor pixel detector Timepix3 was used to track single secondary particles. Measurements were performed in the air, while the detector was positioned out-of-field at a lateral distance of 200 cm parallel with the LINAC exit window. The dose deposited was measured along with the pulse length and the nanostructure of the pulse.
The time of arrival (ToA) of single particles was measured with a resolution of 1.56 ns, while the deposited energy was measured with a resolution of several keV based on the Time over Threshold (ToT) value. The pulse count measured by the Timepix3 detector corresponded with the delivered values, which were measured using an in-flange integrating current transformer (ICT). A linear response (R = 0.999) was established between the delivered beam current and the measured dose at the detector position (orders of nGy). The difference between the average measured and delivered pulse length was ∼0.003(30) μs.
This simple non-invasive method exhibits no limitations on the delivered DPP within the range used during this investigation.
闪疗需要开发先进的质量保证方法和探测器,以准确监测辐射场。本研究介绍了增强型时间分辨率检测系统和方法,该系统和方法用于测量所输送的脉冲数,基于实验室中产生的二次辐射粒子研究单个脉冲的时间结构和每脉冲剂量(DPP)。
将直线加速器(LINAC)产生的20 MeV电子束输送到水模体。使用超高每脉冲剂量电子束,每脉冲剂量范围从约1 Gy到超过7 Gy。在5 Hz的脉冲频率下,脉冲长度范围为1.18 μs至2.88 μs。使用半导体像素探测器Timepix3跟踪单个二次粒子。测量在空气中进行,探测器位于离辐射场外200 cm处,与直线加速器出口窗口平行。测量沉积剂量以及脉冲长度和脉冲的纳米结构。
单个粒子的到达时间(ToA)测量分辨率为1.56 ns,而基于阈值时间(ToT)值测量沉积能量的分辨率为几keV。Timepix3探测器测量的脉冲计数与使用法兰内积分电流互感器(ICT)测量的输送值相对应。在输送的束流与探测器位置处测量的剂量(nGy量级)之间建立了线性响应(R = 0.999)。测量的平均脉冲长度与输送的脉冲长度之间的差异约为0.003(30) μs。
这种简单的非侵入性方法在本研究使用的范围内对所输送的DPP没有限制。