Thermonuclear fusion rates for tritium + deuterium using Bayesian methods

Rafael S. De Souza, S. Reece Boston, Alain Coc, Christian Iliadis

Research output: Contribution to journalArticlepeer-review

21 Scopus citations

Abstract

The H3(d,n)He4 reaction has a large low-energy cross section and will likely be utilized in future commercial fusion reactors. This reaction also takes place during Big Bang nucleosynthesis. Studies of both scenarios require accurate and precise fusion rates. To this end, we implement a one-level, two-channel R-matrix approximation into a Bayesian model. Our main goals are to predict reliable astrophysical S-factors and to estimate R-matrix parameters using the Bayesian approach. All relevant parameters are sampled in our study, including the channel radii, boundary condition parameters, and data set normalization factors. In addition, we take uncertainties in both measured bombarding energies and S-factors rigorously into account. Thermonuclear rates and reactivities of the H3(d,n)He4 reaction are derived by numerically integrating the Bayesian S-factor samples. The present reaction rate uncertainties at temperatures between 1.0 MK and 1.0 GK are in the range of 0.2% to 0.6%. Our reaction rates differ from previous results by 2.9% near 1.0 GK. Our reactivities are smaller than previous results, with a maximum deviation of 2.9% near a thermal energy of 4 keV. The present rate or reactivity uncertainties are more reliable compared to previous studies that did not include the channel radii, boundary condition parameters, and data set normalization factors in the fitting. Finally, we investigate previous claims of electron screening effects in the published H3(d,n)He4 data. No such effects are evident and only an upper limit for the electron screening potential can be obtained.

Original languageEnglish
Article number014619
JournalPhysical Review C
Volume99
Issue number1
DOIs
StatePublished - 2019
Externally publishedYes

Funding

We would like to thank Caleb Marshall for helpful comments. This work was supported in part by NASA under the Astrophysics Theory Program Grant No. 14-ATP14-0007, and the U.S. DOE under Contracts No. DE-FG02-97ER41041 (UNC) and No. DE-FG02-97ER41033 (TUNL).

FundersFunder number
U.S. Department of EnergyDE-FG02-97ER41041
National Aeronautics and Space Administration14-ATP14-0007
University of North Carolina

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