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Application of Neutron Multiplicity Counting Experiments to Optimal Cross-Section Adjustments

机译:中子多重计数实验在最佳截面调整中的应用

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This paper presents the first application of model calibration to neutron multiplicity counting (NMC) experiments for cross-section optimization that is informed by adjoint-based sensitivity analysis (SA) and first-order uncertainty quantification (UQ). We summarize previous work on SA applied to NMC and describe notable modifications and additions. We give the procedure for first-order UQ and Bayesian-inference-based parameter estimation (PE). We then discuss model calibration applied to NMC of a 4.5-kg sphere of weapons-grade, alpha-phase plutonium metal (the BeRP ball) with the nPod neutron multiplicity counter. For the BeRP ball in bare and polyethylene-reflected configurations, we discuss the sensitivity of the first- and second-moment detector responses (i.e., first and second moments of the NMC distribution, respectively) to the cross sections. We describe the sources of uncertainty in the measured and simulated responses. Specifically, uncertainty in the measured responses is due to both random and systematic sources. Uncertainty in the simulated responses is due to the cross-section covariances. We describe in detail the adjustment to the cross sections and cross-section covariances due to the optimization. Due to the contribution of systematic uncertainties to the measured response uncertainties, the adjustment to the cross sections is similar in trend but larger in magnitude compared to that recommended by previous work. We compare the measured responses to responses simulated with nominal and optimized cross sections, demonstrating that the best-estimate cross sections produce simulations of NMC experiments that are more accurate with reduced uncertainty.
机译:本文介绍了模型校准在中子多重性计数(NMC)实验中的首次应用,该实验通过基于伴随的灵敏度分析(SA)和一阶不确定性量化(UQ)进行截面优化。我们总结了以前应用于NMC的SA的工作,并描述了显着的修改和添加。我们给出一阶UQ和基于贝叶斯推理的参数估计(PE)的过程。然后,我们讨论使用nPod中子多重计数器将模型校准应用于4.5公斤级武器级α相p金属(BeRP球)的NMC。对于裸露和聚乙烯反射配置的BeRP球,我们讨论了第一和第二矩检测器响应(即分别为NMC分布的第一和第二矩)对横截面的灵敏度。我们描述了测量和模拟响应中不确定性的来源。具体而言,测量响应的不确定性是由于随机和系统来源造成的。模拟响应的不确定性归因于横截面协方差。由于优化,我们将详细描述对横截面和横截面协方差的调整。由于系统不确定性对测得的响应不确定性的影响,与先前工作建议的相比,对横截面的调整趋势相似,但幅度较大。我们将测量的响应与标称横截面和优化横截面模拟的响应进行比较,表明最佳估计横截面产生的NMC实验模拟更加准确,并且不确定性降低。

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