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Phonon-based mesh optimization for the Monte Carlo on-the-fly thermal scattering temperature fit coefficients

机译:蒙特卡洛飞行中热散射温度拟合系数的基于声子的网格优化

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摘要

In a series of papers, we have introduced a new sampling method for Monte Carlo codes for the low-energy secondary scattering parameters that greatly reduces data storage requirements. The method is based on the temperature dependence of the energy transfer (beta) and squared momentum transfer (alpha) between a neutron and a target nuclide. Cumulative distribution functions (CDFs) in beta and alpha are constructed for a range of temperatures on a mesh of incident energies in the thermal range and temperature fits are created for beta and alpha at discrete CDF probability lines. The secondary energy and angle distributions generated from the fit coefficients showed good agreement with the standard Monte Carlo sampling. However, some discrepancies still existed because the CDF probability mesh values were selected uniformly and arbitrarily. In this paper, a physics-based approach for optimally selecting the CDF probability meshes for the on-the-fly sampling method is introduced, using bound carbon in graphite as the example nuclide. This approach is based on the structure of the phonon frequency distribution of thermal excitations. From the study, it was determined that low (<0.1) and high (>0.9) beta CDF probabilities are important to the structure of the beta probability density functions (PDFs) while very low (<1 x 10(-4)) alpha CDF probabilities are important to the structure of the alpha PDFs. The final meshes contain 200 probability values for both beta and alpha. This results in 14.5 MB of total data storage for the on-the-fly coefficients which are used for any temperature realization. This is a significant reduction in data storage from current methods that require around 25 MB per temperature. (C) 2016 Elsevier B.V. All rights reserved.
机译:在一系列论文中,我们针对低能量二次散射参数引入了一种新的蒙特卡洛代码采样方法,该方法大大降低了数据存储需求。该方法基于中子与目标核素之间能量转移(β)和动量平方(α)的温度依赖性。在热能范围内的入射能量网格上,针对一定温度范围内的温度范围,构造了beta和alpha的累积分布函数(CDF),并在离散的CDF概率线上为beta和alpha创建了温度拟合。由拟合系数生成的二次能量和角度分布与标准蒙特卡洛采样显示出良好的一致性。但是,由于CDF概率网格值是均匀且任意选择的,因此仍然存在一些差异。本文介绍了一种基于物理的方法,它以石墨中的键合碳为示例核素,为动态采样方法最佳选择了CDF概率网格。该方法基于热激发的声子频率分布的结构。从研究中可以确定,低(<0.1)和高(> 0.9)的beta CDF概率对beta概率密度函数(PDFs)的结构很重要,而非常低(<1 x 10(-4))alpha CDF概率对于alpha PDF的结构很重要。最终的网格包含beta和alpha的200个概率值。这样就产生了用于实时系数的14.5 MB的总数据存储量,可用于任何温度实现。与目前每个温度大约需要25 MB的方法相比,这大大减少了数据存储量。 (C)2016 Elsevier B.V.保留所有权利。

著录项

  • 来源
    《Nuclear Engineering and Design》 |2016年第ptab期|70-80|共11页
  • 作者

    Pavlou Andrew T.; Ji Wei;

  • 作者单位

    Rensselaer Polytech Inst, Dept Mech Aerosp & Nucl Engn, 110 8th St,JEC 5040, Troy, NY 12180 USA;

    Rensselaer Polytech Inst, Dept Mech Aerosp & Nucl Engn, 110 8th St,JEC 5040, Troy, NY 12180 USA;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-18 00:41:48

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