Astrophysical $^{3}{\rm He}(\alpha, \gamma)^{7}{\rm Be}$ and $^{3}{\rm H}(\alpha,\gamma)^{7}{\rm Li}$ direct capture reactions in a potential model approach
E.M. Tursunov, S.A. Turakulov, A.S. Kadyrov

TL;DR
This study models the astrophysical reactions $^{3}{ m He}( ext{alpha}, ext{gamma})^{7}{ m Be}$ and $^{3}{ m H}( ext{alpha}, ext{gamma})^{7}{ m Li}$ using a potential model, successfully reproducing experimental data and properties of the involved nuclei.
Contribution
The paper introduces a simple Gaussian potential model that accurately describes both capture reactions and related nuclear properties without additional parameter adjustments.
Findings
The E1-transition from s-wave to p-waves dominates the capture reactions.
The model fits the $^{3}{ m He}( ext{alpha}, ext{gamma})^{7}{ m Be}$ S-factor data at low energies.
The potential model successfully reproduces experimental data for both mirror reactions.
Abstract
The astrophysical and direct capture processes are studied in the framework of the two-body model with the potentials of a simple Gaussian form, which describe correctly the phase-shifts in the s-, p-, d-, and f-waves, as well as the binding energy and the asymptotic normalization constant of the ground and the first excited bound states. It is shown that the E1-transition from the initial s-wave to the final p-waves is strongly dominant in both capture reactions. On this basis the s-wave potential parameters are adjusted to reproduce the new data of the LUNA collaboration around 100 keV and the newest data at the Gamov peak estimated with the help of the observed neutrino fluxes from the Sun, (23 keV)=0.5480.054 keV b for the astrophysical S-factor of the…
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