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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:平均提示中子数据的点对点模型描述作为裂变片段总动能的函数

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The experimental data of average prompt neutron multiplicity as a function of total kinetic energy of fragments (TKE) exhibit, especially in the case of ~(252)Cf(SF), different slopes dTKE/dv and different behaviours at low TKE values. The Point-by-Point (PbP) model can describe these different behaviours. The higher slope dTKE/dv and the flattening of at low TKE exhibited by a part of experimental data sets is very well reproduced when the PbP multi-parametric matrix v(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 v(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: ~(252)Cf(SF), ~(235)U (n_(th),f) and ~(239)Pu(nth,f). In the case of ~(234)U(n,f) for the first time it was possible to calculate (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/dv does not vary with the incident energy and the flattening of 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:作为片段(TKE)表现出的总动能的平均迅速节奏的实验数据,特别是在〜(252)CF(SF)的情况下,不同的斜坡DTKE / DV和低TKE的不同行为价值观。点点(PBP)模型可以描述这些不同的行为。较高斜率dTKE / DV和在低TKE通过试验的数据集的一部分显示出非常良好再现当PBP多参数矩阵V(A,TKE)进行平均双分布Y(A的平坦化,tke)。当在单个分布y(a)上平均相同的矩阵V(a,tke)时,在其他数据集呈现的整个TKE范围内的下斜率和几乎线性行为很好地描述。在SCM中的平均提示中子能量作为TKE的函数的情况下,通过在Y(a,tke)和y(a)上平均相同的Pbp矩阵ε(a,tke)来获得不同的dtke /dε斜率。结果举例说明了三种裂变系统,其有利于实验数据作为TKE的功能:〜(252)CF(SF),〜(235)U(N_(TH),F)和〜(239)PU(NTH,F )。在〜(234)U(N,F)的首次它在许多入射能量通过平均所述的PBP多参数矩阵可以计算(TKE)和<ε>(TKE)的情况下最近在IRMM测量的实验y(A,TKE)分布在0.3-5 meV范围内的14个入射能。结果表明,斜坡Dtke / DV不随着入射能量而变化,并且在低TKE值下的扁平化在低入射能中更加明显。由PBP处理允许使用最可能的碎片方法,在与PBP和Monte Carlo治疗相比非常短的计算时间中提供极大的优点,从而利用最可能的碎片方法,从而利用最可能的碎片方法。

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