| Abstrakt: |
The uncertainties of fission product (FP) inventories in lattice physics depletion and cooling calculations were compared from the viewpoints of generation approaches of FP yield (FPY) covariance matrix and the numerical difference in FPY uncertainties between JENDL-4.0 and ENDF/B-VIII.0. The individual influences of major parent heavy nuclides were also confirmed. Single mass chain (SMC) and generalized least square (GLS) approaches were used to generate the covariance matrix of independent FPYs (IFPYs). It was shown that the FP inventory uncertainty based on the GLS approach was nearly identical or smaller than that based on the SMC approach. A significant difference in uncertainties of 109Ag, 135I, 135Xe, and 147Sm inventories was observed between JENDL-4.0- and ENDF/B-VIII.0-based uncertainty analysis results. The breakdown of individual influences of major parent heavy nuclides revealed that such discrepancies were due to differences in cumulative FPY (CFPY) uncertainty in 109Ag and 147Sm and the modification of IFPY uncertainty in 135I and 135Xe, which were obtained by calculating the covariance components using the GLS approach. Consequently, this study provided a crucial perspective regarding the difference in CFPY uncertainty and modification of IFPY uncertainty due to covariance matrix generation. [ABSTRACT FROM AUTHOR] |
