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Updated Beam Parameters for Monte Carlo Simulation of Five Varian Megavoltage Photon Beams (4, 6,10,15 and 18 MV)

机译:更新的光束参数用于五个Varian兆伏光子光束(4、6、10、15和18 MV)的蒙特卡罗模拟

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Significant discrepancies between Monte Carlo dose calculations and measurements for the Varian 18 MV photon beam with a large field size (40 X 40 cm~2) were reported by different investigators. Chibani and Ma used the GEPTS Monte Carlo code to investigate these discrepancies. They suggested that geometrical data used to model the linac head, and more precisely the primary collimator, are inaccurate. Their findings were later confirmed by the manufacturer: the primary collimator entrance and exit radii are 2 mm larger than expected. More recently, the manufacturer made available new detailed drawings for (i) the tungsten and lead shielding components located between the monitor chamber and the Y jaws, (ii) the mirror frame and the (iii) tungsten base plate located downstream of the X jaws. The purpose of this study is to investigate the impact of more precise linac head geometry on dose distributions and also to extend the results we obtained for the 18 MV photon beam (Med. Phys. Vol. 34 2007 p. 1206) to other energies: 4, 6, 10, and 15 MV. Contrary to most publications, the beam parameters (energy spectrum and lateral intensity distribution of primary electrons) are checked for a wide range of field sizes (2x2 cm2 to 40x40 cm2), not only for 10x10 cm2. Our preliminary results show that beam models can be tuned to mach measured depth dose and dose profile distributions within 1% difference for any depth larger than 1 cm. Monte Carlo simulation of the ionization chamber response shows that difference between calculated and measured percent depth ionizations can be reduced to less than 3% even at zero depth where half of the ionization chamber is outside the phantom.
机译:不同研究人员报告了大视野尺寸(40 X 40 cm〜2)的Varian 18 MV光子束的蒙特卡洛剂量计算与测量值之间存在显着差异。 Chibani和Ma使用GEPTS蒙特卡洛代码研究了这些差异。他们认为,用于建模直线加速器头部(更确切地说是主准直器)的几何数据是不准确的。制造商随后证实了他们的发现:准直仪的主入口和出口半径比预期的大2毫米。最近,制造商提供了新的详细图纸,用于(i)位于监控室和Y型夹爪之间的钨和铅屏蔽组件,(ii)镜框和(iii)位于X夹爪下游的钨基板。 。这项研究的目的是研究更精确的直线加速器头部几何形状对剂量分布的影响,并将我们对18 MV光子束(Med。Phys。Vol。34 2007 p。1206)获得的结果扩展到其他能量: 4、6、10和15 MV。与大多数出版物相反,对于广泛的场尺寸(2x2 cm2到40x40 cm2),不仅是10x10 cm2,还检查了电子束参数(能量谱和一次电子的横向强度分布)。我们的初步结果表明,对于任何大于1 cm的深度,光束模型都可以调整到马赫测得的深度剂量和1%差异之内的剂量分布。电离室响应的蒙特卡罗模拟显示,即使在一半深度的电离室位于体模之外的零深度处,所计算出的深度电离与测量的实测百分比电离之间的差异也可以减小至小于3%。

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