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用于 UHDR 质子笔形束中不同剂量和剂量率估计的实验比较的定量、实时闪烁成像。

Quantitative, real-time scintillation imaging for experimental comparison of different dose and dose rate estimations in UHDR proton pencil beams.

机构信息

Thayer School of Engineering, Dartmouth College, Hanover, New Hampshire, USA.

Department of Radiation Oncology, University of Alabama at Birmingham, Birmingham, Alabama, USA.

出版信息

Med Phys. 2024 Sep;51(9):6402-6411. doi: 10.1002/mp.17247. Epub 2024 Jun 11.

Abstract

BACKGROUND

Ultra-high dose rate radiotherapy (UHDR-RT) has demonstrated normal tissue sparing capabilities, termed the FLASH effect; however, available dosimetry tools make it challenging to characterize the UHDR beams with sufficiently high concurrent spatial and temporal resolution. Novel dosimeters are needed for safe clinical implementation and improved understanding of the effect of UHDR-RT.

PURPOSE

Ultra-fast scintillation imaging has been shown to provide a unique tool for spatio-temporal dosimetry of conventional cyclotron pencil beam scanning (PBS) deliveries, indicating the potential use for characterization of UHDR PBS proton beams. The goal of this work is to introduce this novel concept and demonstrate its capabilities in recording high-resolution dose rate maps at FLASH-capable proton beam currents, as compared to log-based dose rate calculation, internally developed UHDR beam simulation, and a fast point detector (EDGE diode).

METHODS

The light response of a scintillator sheet located at isocenter and irradiated by PBS proton fields (40-210 nA, 250 MeV) was imaged by an ultra-fast iCMOS camera at 4.5-12 kHz sampling frequency. Camera sensor and image intensifier gain were optimized to maximize the dynamic range; the camera acquisition rate was also varied to evaluate the optimal sampling frequency. Large field delivery enabled flat field acquisition for evaluation of system response homogeneity. Image intensity was calibrated to dose with film and the recorded spatio-temporal data was compared to a PPC05 ion chamber, log-based reconstruction, and EDGE diode. Dose and dose rate linearity studies were performed to evaluate agreement under various beam conditions. Calculation of full-field mean and PBS dose rate maps were calculated to highlight the importance of high resolution, full-field information in UHDR studies.

RESULTS

Camera response was linear with dose (R = 0.997) and current (R2 = 0.98) in the range from 2-22 Gy and 40-210 nA, respectively, when compared to ion chamber readings. The deviation of total irradiation time calculated with the imaging system from the log file recordings decreased from 0.07% to 0.03% when imaging at 12 kfps versus 4.5 kfps. Planned and delivered spot positions agreed within 0.2 0.1 mm and total irradiation time agreed within 0.2 0.2 ms when compared with the log files, indicating the high concurrent spatial and temporal resolution. For all deliveries, the PBS dose rate measured at the diode location agreed between the imaging and the diode within 3% 2% and with the simulation within 5% 3% CONCLUSIONS: Full-field mapping of dose and dose rate is imperative for complete understanding of UHDR PBS proton dose delivery. The high linearity and various spatiotemporal metric reporting capabilities confirm the continued use of this camera system for UHDR beam characterization, especially for spatially resolved dose rate information.

摘要

背景

超高剂量率放疗(UHDR-RT)已显示出对正常组织的保护能力,称为FLASH 效应;然而,现有的剂量测量工具使得很难以足够高的空间和时间分辨率来描述 UHDR 光束。需要新型剂量计来实现安全的临床应用,并深入了解 UHDR-RT 的效果。

目的

超快闪烁成像是对传统回旋加速器笔形束扫描(PBS)输送的时空剂量学进行独特的工具,表明其在 UHDR PBS 质子束特性描述方面具有潜在用途。这项工作的目的是引入这一新概念,并展示其在记录高分辨率剂量率图方面的能力,这些图是在 FLASH 能力的质子束电流下记录的,与基于对数的剂量率计算、内部开发的 UHDR 光束模拟和快速点探测器(EDGE 二极管)相比。

方法

位于等中心的闪烁片被 PBS 质子场(40-210 nA,250 MeV)照射,由超快 iCMOS 相机以 4.5-12 kHz 的采样频率进行成像。相机传感器和像增强器增益经过优化,以最大限度地提高动态范围;还改变了相机采集率,以评估最佳采样频率。大的场输送实现了平面场采集,以评估系统响应的均匀性。通过胶片对图像强度进行剂量标定,并将记录的时空数据与 PPC05 离子室、基于对数的重建和 EDGE 二极管进行比较。进行剂量和剂量率线性研究,以评估在不同光束条件下的一致性。计算全场平均和 PBS 剂量率图,以突出在 UHDR 研究中高分辨率、全场信息的重要性。

结果

当与离子室读数相比时,相机响应在 2-22 Gy 和 40-210 nA 的范围内分别与剂量(R = 0.997)和电流(R2 = 0.98)呈线性关系。当以 12 kfps 进行成像而不是 4.5 kfps 时,与日志文件记录相比,总辐照时间的计算偏差从 0.07%减少到 0.03%。与日志文件相比,计划和输送的光斑位置的偏差在 0.2 0.1 毫米内,总辐照时间的偏差在 0.2 0.2 毫秒内,表明具有高的同时空间和时间分辨率。对于所有输送,二极管位置测量的 PBS 剂量率在成像和二极管之间的差异在 3% 2%以内,与模拟结果的差异在 5% 3%以内。

结论

完全理解 UHDR PBS 质子剂量输送,需要对剂量和剂量率进行全场映射。高线性度和各种时空度量报告功能证实了该相机系统在 UHDR 光束特性描述方面的持续使用,特别是对于空间分辨率剂量率信息。

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