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Application of the GBFP Method to Electron Partial-Wave Expansion Elastic Scattering Differential Cross Sections Within the Geant4 Toolkit

机译:GBFP方法在Geant4工具包内电子部分波扩展弹性散射微分截面中的应用

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摘要

Analog Monte Carlo simulation of electrons in complex material geometries is generally impractical because the long range Coulomb interactions result in highly peaked differential cross sections (DCS) for scattering and energy-loss and extremely small collision mean free paths (mfp). The condensed history (CH) Monte Carlo method attempts to alleviate this limitation by advancing electrons in fixed steps and sampling angular deflections and energy losses from precomputed distributions obtained from approximate solutions to the underlying transport equation that are valid only for thin layers. Though CH is efficient and is widely employed in production codes (ITS, MCNP, EGS, Geant), step size restrictions and inconsistent handling of material and free surface boundaries limit the ultimate accuracy possible with this approach, especially in applications to highly heterogeneous media.
机译:通常,在复杂材料几何形状中对电子进行模拟蒙特卡洛模拟是不切实际的,因为长距离库仑相互作用会导致散射和能量损失的峰化微分截面(DCS)高度峰值,并且碰撞平均自由程(mfp)极小。凝聚历史(CH)蒙特卡罗方法试图通过以固定步长推进电子并从预先计算的分布中采样角偏转和能量损失来缓解此限制,这些预计算分布是从仅对薄层有效的基础传输方程的近似解中获得的。尽管CH是高效的并且已广泛用于生产代码(ITS,MCNP,EGS,Geant)中,但是步长限制以及对材料和自由表面边界的不一致处理限制了这种方法的最终精度,尤其是在高度异构介质中。

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  • 会议地点 Knoxville TN(US)
  • 作者单位

    University of New Mexico: Dept. of Chemical and Nuclear Engineering, Farris Engineering Center, Albuquerque, New Mexico, 87131;

    University of New Mexico: Dept. of Chemical and Nuclear Engineering, Farris Engineering Center, Albuquerque, New Mexico, 87131;

    Sandia National Laboratories: P.O. Box 5800, Albuquerque, New Mexico, 87185-1179;

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  • 正文语种 eng
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