Ding Aiping, Xing Lei, Han Bin
Department of Radiation Oncology, Stanford University School of Medicine, Stanford, Calilfornia 94305.
Med Phys. 2015 Jul;42(7):4190-8. doi: 10.1118/1.4922400.
To develop an efficient and robust tool for output measurement and absolute dose verification of electron beam therapy by using a high spatial-resolution and high frame-rate amorphous silicon flat panel electronic portal imaging device (EPID).
The dosimetric characteristics of the EPID, including saturation, linearity, and ghosting effect, were first investigated on a Varian Clinac 21EX accelerator. The response kernels of the individual pixels of the EPID to all available electron energies (6, 9, 12, 16, and 20 MeV) were calculated by using Monte Carlo (MC) simulations, which formed the basis to deconvolve an EPID raw images to the incident electron fluence map. The two-dimensional (2D) dose distribution at reference depths in water was obtained by using the constructed fluence map with a MC simulated pencil beam kernel with consideration of the geometric and structural information of the EPID. Output factor measurements were carried out with the EPID at a nominal source-surface distance of 100 cm for 2 × 2, 3 × 3, 6 × 6, 10 × 10, and 15 × 15 cm(2) fields for all available electron energies, and the results were compared with that measured in a solid water phantom using film and a Farmer-type ion chamber. The dose distributions at a reference depth specific to each energy and the flatness and symmetry of the 10 × 10 cm(2) electron beam were also measured using EPID, and the results were compared with ion chamber array and water scan measurements. Finally, three patient cases with various field sizes and irregular cutout shapes were also investigated.
EPID-measured dose changed linearly with the monitor units and showed little ghosting effect for dose rate up to 600 MU/min. The flatness and symmetry measured with the EPID were found to be consistent with ion chamber array and water scan measurements. The EPID-measured output factors for standard square fields of 2 × 2, 3 × 3, 6 × 6, 10 × 10, 15 × 15 cm(2) agreed with film and ion chamber measurements. The average discrepancy between EPID and ion chamber/film measurements was 0.81% ± 0.60% (SD) and 1.34% ± 0.75%, respectively. For the three clinical cases, the difference in output between the EPID- and ion chamber array measured values was found to be 1.13% ± 0.11%, 0.54% ± 0.10%, and 0.74% ± 0.11%, respectively. Furthermore, the γ-index analysis showed an excellent agreement between the EPID- and ion chamber array measured dose distributions: 100% of the pixels passed the criteria of 3%/3 mm. When the γ-index was set to be 2%/2 mm, the pass rate was found to be 99.0% ± 0.07%, 98.2% ± 0.14%, and 100% for the three cases.
The EPID dosimetry system developed in this work provides an accurate and reliable tool for routine output measurement and dosimetric verification of electron beam therapy. Coupled with its portability and ease of use, the proposed system promises to replace the current film-based approach for fast and reliable assessment of small and irregular electron field dosimetry.
通过使用高空间分辨率和高帧率的非晶硅平板电子射野影像装置(EPID),开发一种用于电子束治疗输出剂量测量和绝对剂量验证的高效且可靠的工具。
首先在瓦里安Clinac 21EX加速器上研究了EPID的剂量学特性,包括饱和度、线性度和残影效应。通过蒙特卡罗(MC)模拟计算了EPID各个像素对所有可用电子能量(6、9、12、16和20 MeV)的响应核,这构成了将EPID原始图像反卷积为入射电子注量图的基础。利用构建的注量图以及考虑了EPID几何和结构信息的MC模拟笔形束核,获得了水中参考深度处的二维(2D)剂量分布。在标称源皮距为100 cm的情况下,使用EPID对所有可用电子能量下的2×2、3×3、6×6、10×10和15×15 cm²射野进行输出因子测量,并将结果与在固体水模体中使用胶片和 Farmer 型电离室测量的结果进行比较。还使用EPID测量了每种能量特定参考深度处的剂量分布以及10×10 cm²电子束的平坦度和对称性,并将结果与电离室阵列和水扫描测量结果进行比较。最后,还研究了三个具有不同射野大小和不规则遮挡形状的患者病例。
EPID测量的剂量与监测单位呈线性变化,对于高达600 MU/min的剂量率,残影效应很小。发现用EPID测量的平坦度和对称性与电离室阵列和水扫描测量结果一致。EPID测量的2×2、3×3、6×6、10×10、15×15 cm²标准方形射野的输出因子与胶片和电离室测量结果一致。EPID与电离室/胶片测量结果之间的平均差异分别为0.81%±0.60%(标准差)和1.34%±0.75%。对于三个临床病例,发现EPID和电离室阵列测量值之间的输出差异分别为1.13%±0.11%、0.54%±0.10%和0.74%±0.11%。此外,γ指数分析表明EPID和电离室阵列测量的剂量分布之间具有极好的一致性:100%的像素通过了3%/3 mm的标准。当γ指数设置为2%/2 mm时,三个病例的通过率分别为99.0%±0.07%、98.2%±0.14%和100%。
本研究中开发的EPID剂量测定系统为电子束治疗的常规输出剂量测量和剂量验证提供了一种准确可靠的工具。结合其便携性和易用性,所提出的系统有望取代当前基于胶片的方法,用于快速可靠地评估小的和不规则电子射野剂量学。