Medical Radiation Physics, Carl v. Ossietzky University, Oldenburg 26127, Germany and Department for Radiation Oncology, Pius Hospital, Oldenburg 26121, Germany.
Radiotherapy Department, General Hospital, Celle 29223, Germany.
Med Phys. 2014 Feb;41(2):021707. doi: 10.1118/1.4861098.
The purpose of this study is the correction of the lateral scanner artifact, i.e., the effect that, on a large homogeneously exposed EBT3 film, a flatbed scanner measures different optical densities at different positions along the x axis, the axis parallel to the elongated light source. At constant dose, the measured optical density profiles along this axis have a parabolic shape with significant dose dependent curvature. Therefore, the effect is shortly called the parabola effect. The objective of the algorithm developed in this study is to correct for the parabola effect. Any optical density measured at given position x is transformed into the equivalent optical density c at the apex of the parabola and then converted into the corresponding dose via the calibration of c versus dose.
For the present study EBT3 films and an Epson 10000XL scanner including transparency unit were used for the analysis of the parabola effect. The films were irradiated with 6 MV photons from an Elekta Synergy accelerator in a RW3 slab phantom. In order to quantify the effect, ten film pieces with doses graded from 0 to 20.9 Gy were sequentially scanned at eight positions along the x axis and at six positions along the z axis (the movement direction of the light source) both for the portrait and landscape film orientations. In order to test the effectiveness of the new correction algorithm, the dose profiles of an open square field and an IMRT plan were measured by EBT3 films and compared with ionization chamber and ionization chamber array measurement.
The parabola effect has been numerically studied over the whole measuring field of the Epson 10000XL scanner for doses up to 20.9 Gy and for both film orientations. The presented algorithm transforms any optical density at position x into the equivalent optical density that would be measured at the same dose at the apex of the parabola. This correction method has been validated up to doses of 5.2 Gy all over the scanner bed with 2D dose distributions of an open square photon field and an IMRT distribution.
The algorithm presented in this study quantifies and corrects the parabola effect of EBT3 films scanned in commonly used commercial flatbed scanners at doses up to 5.2 Gy. It is easy to implement, and no additional work steps are necessary in daily routine film dosimetry.
本研究的目的是纠正侧向扫描仪伪影,即当在大面积均匀曝光的 EBT3 胶片上,平板扫描仪在与细长光源平行的 x 轴(即横轴)上的不同位置测量不同的光密度时,所产生的影响。在剂量恒定的情况下,该轴上的测量光密度曲线呈抛物线形状,且曲率与剂量显著相关。因此,该影响通常被称为抛物线效应。本研究中开发的算法的目的是纠正该抛物线效应。在给定位置 x 测量的任何光密度都转换为抛物线顶点处的等效光密度 c,然后通过 c 与剂量的校准将其转换为相应的剂量。
本研究使用 EBT3 胶片和 Epson 10000XL 扫描仪(包括透明单元)分析抛物线效应。胶片在 RW3 平板体模中用 6MV 光子从 Elekta Synergy 加速器进行照射。为了量化该影响,将十个剂量从 0 到 20.9Gy 逐渐递增的胶片片在 x 轴的八个位置和 z 轴(光源移动方向)的六个位置处,分别沿胶片的横、竖方向进行顺序扫描。为了测试新校正算法的有效性,使用 EBT3 胶片测量了一个开放正方形射野和一个调强放疗计划的剂量分布,并与电离室和电离室矩阵测量进行了比较。
已经对 Epson 10000XL 扫描仪的整个测量场进行了数值研究,研究了高达 20.9Gy 的剂量以及两种胶片方向的抛物线效应。所提出的算法将任何位置 x 的光密度转换为在相同剂量下在抛物线顶点处测量的等效光密度。该校正方法已在整个扫描仪床面上进行了验证,验证剂量高达 5.2Gy,验证了开放正方形光子射野和调强放疗分布的 2D 剂量分布。
本研究中提出的算法在高达 5.2Gy 的剂量下,量化并校正了在常用商用平板扫描仪中扫描的 EBT3 胶片的抛物线效应。它易于实现,在日常胶片剂量学中不需要额外的工作步骤。