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首页> 外文期刊>International Journal of Applied Engineering Research >Monte Carlo calculation of 6 MV Varian Linac photon beam Spectral characteristics using the BEAM code
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Monte Carlo calculation of 6 MV Varian Linac photon beam Spectral characteristics using the BEAM code

机译:使用BEAM代码对6 MV Varian Linac光子束光谱特性进行蒙特卡洛计算

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In this study the BEAMnrc Monte Carlo (MC) code is used to simulate 6 MV photon beam as the MC methods are consider to be most reliable and accurate to evaluate the radiation beam characteristics. In this work the MC simulation model is used to calculate depth-dose curves and contribution of contaminant electron to it. We also calculated photon spectra, photon average energy distributions, photon energy fluence spectra, contaminant electron spectra at 100 cm source to surface distance. The sensitivity of these parameters has been analyzed in detail. The contribution of electrons to the central-axis depth-dose was calculated and it was observed that its contribution is less than 7% of maximum total dose at surface, while at the depth of maximum dose (d_(max)) its contribution was less than 3% of maximum total dose for 10×10 cm~2 field sizes. The photon energy fluence spectra are separated into direct and scatter components from the primary collimator, flattening filter and the adjustable collimators. The contribution of direct photons to the total photon energy fluence is about 97% and the scatter contributions to the total photon energy fluence from the primary collimator and flattening filter are typically less than 3% and scatter contributions from jaws is less than 0.30% to the total photon energy fluence for 10×10 cm~2 fields size. The calculated and measured depth-dose data agree within 1% of local dose, and 1.0 mm in depth at all depths and field sizes which gave enough confidence that MC Simulations could be used to simulate the 6 MV photon beam. Our study shows that both photon and electron fluence spectra strongly depend upon field size. Most of the scatter energy fluence of photon comes from flattening filter and primary collimator. Beam hardening effects of flattening filter have also been verified by the study of average energy distribution.
机译:在这项研究中,BEAMnrc Monte Carlo(MC)代码用于模拟6 MV光子束,因为MC方法被认为是评估辐射束特性的最可靠,最准确的方法。在这项工作中,MC模拟模型用于计算深度-剂量曲线以及污染物电子对其的贡献。我们还计算了100 cm源到表面距离的光子光谱,光子平均能量分布,光子能量注量光谱,污染物电子光谱。这些参数的敏感性已被详细分析。计算了电子对中心轴深度剂量的贡献,观察到电子的贡献小于表面最大总剂量的7%,而在最大剂量深度(d_(max))时,电子的贡献较小对于10×10 cm〜2场大小,最大总剂量的3%以上。光子能量通量光谱从主准直仪,展平滤波器和可调准直仪分为直接分量和散射分量。直接光子对总光子能量通量的贡献约为97%,主准直仪和展平滤波器对总光子能量通量的散射贡献通常小于3%,而从下巴到对光子的散射贡献小于0.30% 10×10 cm〜2场大小的总光子能量通量。计算得出的和测量的深度剂量数据在局部剂量的1%之内,并且在所有深度和视野大小下的深度均为1.0毫米,这给MC模拟可以用来模拟6 MV光子束提供了足够的信心。我们的研究表明,光子注量谱和电子注量谱都强烈取决于场大小。光子的散射能量通量大部分来自平坦滤波器和主准直器。通过平均能量分布的研究也证明了平坦滤波器的束硬化效果。

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