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Point-by-Point model description of average prompt neutron data as a function of total kinetic energy of fission fragments

机译:平均瞬发中子数据与裂变碎片总动能的逐点模型描述

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The experimental data of average prompt neutron multiplicity as a function of total kinetic energy of fragments ν>(TKE) exhibit, especially in the case of 252Cf(SF), different slopes dTKE/dν and different behaviours at low TKE values. The Point-by-Point (PbP) model can describe these different behaviours. The higher slope dTKE/dν and the flattening of ν> at low TKE exhibited by a part of experimental data sets is very well reproduced when the PbP multi-parametric matrix ν(A,TKE) is averaged over a double distribution Y(A,TKE). The lower slope and the almost linear behaviour over the entire TKE range exhibited by other data sets is well described when the same matrix ν(A,TKE) is averaged over a single distribution Y(A). In the case of average prompt neutron energy in SCM as a function of TKE, different dTKE/dε slopes are also obtained by averaging the same PbP matrix ε(A,TKE) over Y(A,TKE) and over Y(A). The results are exemplified for three fissioning systems benefiting of experimental data as a function of TKE: 252Cf(SF), 235U(nth,f) and 239Pu(nth,f). In the case of 234U(n,f) for the first time it was possible to calculate ν>(TKE) and ε>(TKE) at many incident energies by averaging the PbP multi-parametric matrices over the experimental Y(A,TKE) distributions recently measured at IRMM for 14 incident energies in the range 0.3-5 MeV. The results revealed that the slope dTKE/dν does not vary with the incident energy and the flattening of ν> at low TKE values is more pronounced at low incident energies. The average model parameters dependences on TKE resulted from the PbP treatment allow the use of the most probable fragmentation approach, having the great advantage to provide results at many TKE values in a very short computing time compared to PbP and Monte Carlo treatments.
机译:平均瞬态中子多重性随碎片总动能ν>(TKE)的实验数据显示,特别是在252Cf(SF)的情况下,不同的斜率dTKE /dν和低TKE值下的不同行为。点对点(PbP)模型可以描述这些不同的行为。当将PbP多参数矩阵ν(A,TKE)在双分布Y(A,上平均)时,很好地再现了部分实验数据集表现出的较高斜率dTKE /dν和低TKE下的ν>平坦度。 TKE)。当在单个分布Y(A)上对相同矩阵ν(A,TKE)求平均值时,很好地描述了其他数据集在整个TKE范围内显示的较低斜率和几乎线性的行为。在SCM中平均瞬发中子能量是TKE的函数的情况下,还可以通过对Y(A,TKE)和Y(A)上相同的PbP矩阵ε(A,TKE)求平均值来获得不同的dTKE /dε斜率。该结果以三个裂变系统为例,该裂变系统得益于作为TKE的函数的实验数据:252Cf(SF),235U(nth,f)和239Pu(nth,f)。首次使用234U(n,f)时,可以通过对实验Y(A,TKE)上的PbP多参数矩阵求平均来计算许多入射能量下的ν>(TKE)和ε>(TKE) )最近在IRMM上测量的0.3-5 MeV范围内的14种入射能量的分布。结果表明,斜率dTKE /dν不随入射能量而变化,并且在低TKE值下,ν>的平坦度在低入射能量下更为明显。由PbP处理产生的平均模型参数对TK​​E的依赖性允许使用最可能的碎片化方法,与PbP和Monte Carlo处理相比,具有在非常短的计算时间内以许多TKE值提供结果的巨大优势。

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