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Collimator scatter factor: Monte Carlo and in-air measurements approaches

机译:准直器散射因子:蒙特卡罗和空中测量方法

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Linac output as a function of field sizes has a phantom and a head scatter component. This last term can be measured in-air with appropriate build-up ensuring a complete electron equilibrium and the absence of the contaminant electrons. Equilibrium conditions could be achieved using a build-up cap or a mini-phantom. Monte Carlo simulations in a virtual phantom mimicking a mini-phantom were analysed with the aim of better understanding the setup conditions for measuring the collimator scatter factor that is the head scatter component of the linac output factors. Beams of 6 and 15 MV from a TrueBeam, with size from 4?×?4 to 40?×?40 cm2 were simulated in cylindrical acrylic phantoms 20?cm long, of different diameters, from 0.5 to 4?cm, with the cylinder axis coincident with the beam central axis. The PRIMO package, based on PENELOPE Monte Carlo code, was used. The phase-space files for a Varian TrueBeam linac, provided by the linac vendor, were used for the linac head simulation. Depth dose curves were analysed, and collimator scatter factors estimated at different depth in the different phantom conditions. Additionally, in-air measurements using acyrilic and brass build-up caps, as well as acrylic mini-phantom were acquired for 6 and 18 MV beams from a Varian Clinac DHX. The depth dose curves along the cylinders were compared, showing, in each phantom, very similar curves for all analysed field sizes, proving the correctness in estimating the collimator scatter factor in the mini-phantom, provided to position the detector to a sufficient depth to exclude electron contamination. The results were confirmed by the measurements, where the acrylic build-up cap showed to be inadequate to properly estimate the collimator scatter factors, while the mini-phantom and the brass caps gave reasonable measurements. A better understanding of the beam characteristics inside a virtual mini-phantom through the analysis of depth dose curves, showed the critical points of using the acrylic build-up cap, and suggested the use of the mini-phantom for the collimator scatter factor measurements in the medium-large field size range.
机译:直线加速器输出作为视场大小的函数,具有幻像和头部散射分量。该最后一项可以在空气中以适当的积累进行测量,以确保完全的电子平衡和不存在污染电子。平衡条件可以使用堆积帽或迷你模型来实现。为了更好地了解用于测量准直器散射因子(即直线加速器输出因子的头部散射成分)的设置条件,对模拟微型幻像的虚拟幻象中的Monte Carlo仿真进行了分析。用圆柱体在20厘米长,直径从0.5到4厘米不等的圆柱形丙烯酸模型中模拟TrueBeam发出的6和15 MV光束,尺寸从4?×?4到40?×?40 cm2。轴与光束中心轴重合。使用了基于PENELOPE蒙特卡洛代码的PRIMO软件包。直线加速器供应商提供的Varian TrueBeam直线加速器的相空间文件用于直线加速器头部仿真。分析了深度剂量曲线,并估计了在不同体模条件下不同深度的准直器散射因子。此外,还使用Varian Clinac DHX的6和18 MV光束获得了使用丙烯酸和黄铜组合帽进行的空中测量以及丙烯酸微型模型。比较了沿圆柱体的深度剂量曲线,在每个幻像中显示了所有分析场大小的非常相似的曲线,证明了估计微型幻像中的准直器散射因子的正确性,可以将检测器定位到足够的深度以达到排除电子污染。测量结果证实了这一结果,其中丙烯酸堆积帽不足以正确估计准直器散射因子,而微型幻影和黄铜帽给出了合理的测量值。通过对深度剂量曲线的分析,可以更好地了解虚拟微型体模内的光束特性,显示了使用丙烯酸树脂堆积帽的关键点,并建议在微型准直器散射系数测量中使用微型体模。中大字段大小范围。

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