The Regulated GeAs Cycles with the New 63Ga(p,γ)64Ge and 64Ge(p,γ)65As Reaction Rates and Their Impact on the GS 1826-24 Clocked Bursts and SAX J1808.4-3658 Photospheric Radius Expansion Bursts

Abstract

The 63Ga(p,γ)64Ge and 64Ge(p,γ)65As thermonuclear reactions connect the ZnGa and GeAs cycles by diverting the flow of the rapid proton capture process from 63Ga to 65As. Changes in these two reaction rates regulate the ZnGa and GeAs cycles and may affect the modeled properties matching with the observed counterparts of a type I X-ray burster. We implement the latest 63Ga(p,γ)64Ge and 64Ge(p,γ)65As reaction rates to the state-of-the-art self-consistent one-dimensional multi-zone thermo-hydrodynamic code, KEPLER, to study the influence of these new reaction rates on the models of the GS 1826-24 clocked burster and SAX J1808.4-3658 photospheric radius expansion burster. Both new reaction rates obtained by Lu et al. [Phys. Rev. C 110, 065804 (2024)] are determined from complementing the experimental input with the nuclear spectroscopic information deduced from the full pf-shell space configuration-interaction shell-model calculations. By constraining the models on reproducing the observed burst peak, light-curve profile, fluence, and recurrence time, we find that the impact of the newly measured proton thresholds and respective proton-capture reactions on the burst light-curve profile of the GS 1826-24 clocked burster is, in fact, not as significant as claimed by Zhou et al. [Nat. Phys. 19, 1091 (2023)]. With or without the inclusion of the newly determined reaction rate of the highly influential 22Mg(α,p)25Al reaction, the impact of the new 63Ga(p,γ)64Ge and 64Ge(p,γ)65As reaction rates on SAX J1808.4-3658 photospheric radius expansion bursts is evident. Our finding indicates that the models reproducing the 2002 October epoch of SAX J1808.4-3658 photospheric radius expansion burster is more sensitive to the uncertainties of thermonuclear reaction rates.

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