TY - JOUR
T1 - Bayesian model averaging (BMA) for nuclear data evaluation
AU - Alhassan, E.
AU - Rochman, D.
AU - Schnabel, G.
AU - Koning, A. J.
N1 - Score=10
Publisher Copyright:
© The Author(s), under exclusive licence to China Science Publishing & Media Ltd. (Science Press), Shanghai Institute of Applied Physics, the Chinese Academy of Sciences, Chinese Nuclear Society 2024.
PY - 2024/11
Y1 - 2024/11
N2 - To ensure agreement between theoretical calculations and experimental data, parameters to selected nuclear physics models are perturbed and fine-tuned in nuclear data evaluations. This approach assumes that the chosen set of models accurately represents the ‘true’ distribution of considered observables. Furthermore, the models are chosen globally, indicating their applicability across the entire energy range of interest. However, this approach overlooks uncertainties inherent in the models themselves. In this work, we propose that instead of selecting globally a winning model set and proceeding with it as if it was the ‘true’ model set, we, instead, take a weighted average over multiple models within a Bayesian model averaging (BMA) framework, each weighted by its posterior probability. The method involves executing a set of TALYS calculations by randomly varying multiple nuclear physics models and their parameters to yield a vector of calculated observables. Next, computed likelihood function values at each incident energy point were then combined with the prior distributions to obtain updated posterior distributions for selected cross sections and the elastic angular distributions. As the cross sections and elastic angular distributions were updated locally on a per-energy-point basis, the approach typically results in discontinuities or “kinks” in the cross section curves, and these were addressed using spline interpolation. The proposed BMA method was applied to the evaluation of proton-induced reactions on 58Ni between 1 and 100 MeV. The results demonstrated a favorable comparison with experimental data as well as with the TENDL-2023 evaluation.
AB - To ensure agreement between theoretical calculations and experimental data, parameters to selected nuclear physics models are perturbed and fine-tuned in nuclear data evaluations. This approach assumes that the chosen set of models accurately represents the ‘true’ distribution of considered observables. Furthermore, the models are chosen globally, indicating their applicability across the entire energy range of interest. However, this approach overlooks uncertainties inherent in the models themselves. In this work, we propose that instead of selecting globally a winning model set and proceeding with it as if it was the ‘true’ model set, we, instead, take a weighted average over multiple models within a Bayesian model averaging (BMA) framework, each weighted by its posterior probability. The method involves executing a set of TALYS calculations by randomly varying multiple nuclear physics models and their parameters to yield a vector of calculated observables. Next, computed likelihood function values at each incident energy point were then combined with the prior distributions to obtain updated posterior distributions for selected cross sections and the elastic angular distributions. As the cross sections and elastic angular distributions were updated locally on a per-energy-point basis, the approach typically results in discontinuities or “kinks” in the cross section curves, and these were addressed using spline interpolation. The proposed BMA method was applied to the evaluation of proton-induced reactions on 58Ni between 1 and 100 MeV. The results demonstrated a favorable comparison with experimental data as well as with the TENDL-2023 evaluation.
KW - Bayesian model averaging (BMA)
KW - Covariances
KW - Model parameters
KW - Nuclear data
KW - Nuclear reaction models
KW - TALYS code system
UR - http://www.scopus.com/inward/record.url?scp=85206496542&partnerID=8YFLogxK
U2 - 10.1007/s41365-024-01543-w
DO - 10.1007/s41365-024-01543-w
M3 - Article
AN - SCOPUS:85206496542
SN - 1001-8042
VL - 35
JO - Nuclear Science and Techniques
JF - Nuclear Science and Techniques
IS - 11
M1 - 205
ER -