Abstract:Abstract. In most cases RGB and AGB stars with M≤ 2M destroy Li (which is instead synthesized trough electron-captures on 7 Be). This occurs through the combined operation of mixing processes and proton captures, when H-burning operates close to the envelope. Observed Li abundances are however difficult to explain, as they cover a wide spread. Various uncertainties affect model attempts, but so far the largest one concerns the processes of bound and free ecaptures on 7 Be, hence its life-time, whose known esti… Show more
“…Furthermore, despite these transitions being quark-level processes, they also strongly depend on extra-nuclear factors, such as temperature and electron density, which significantly vary in the layers of evolved stars outside the degenerate core. Indeed, these parameters may affect the ionization degree of the atomic systems where the decay occurs, which in turn modifies the discrete-to-continuum transition ratio (Simonucci et al 2013;Palmerini et al 2016;Vescovi et al 2019).…”
We analyze the
55
134
Cs
→
56
134
Ba and
55
135
Cs
→
56
135
Ba β
− decays, which are crucial production channels for Ba isotopes in asymptotic giant branch (AGB) stars. We calculate, starting from relativistic quantum mechanics, the effects of multichannel scattering onto weak decays, including nuclear and electronic excited states (ESs) populated above ≃10 keV, for both parent and daughter nuclei. We find increases in the half-lives for T > 108 K (by more than a factor of 3 for 134Cs) as compared to previous works based on systematics. We also discuss our method in view of these previous calculations. An important impact on half-lives comes from nuclear ES decays, while including electronic temperatures yields further increases of about 20% at energies of 10–30 keV, typical of AGB stars of moderate mass (M ≲ 8 M
⊙). Despite properly considering these effects, the new rates remain sensitively lower than the Takahashi & Yokoi values, implying longer half-lives at least above 8–9 keV. Our rate predictions are in substantial accord with recent results based on the shell model, and strongly modify branching ratios along the s-process path previously adopted. With our new rate, nucleosynthesis models well account for the isotopic admixtures of Ba in presolar SiC grains and in the Sun.
“…Furthermore, despite these transitions being quark-level processes, they also strongly depend on extra-nuclear factors, such as temperature and electron density, which significantly vary in the layers of evolved stars outside the degenerate core. Indeed, these parameters may affect the ionization degree of the atomic systems where the decay occurs, which in turn modifies the discrete-to-continuum transition ratio (Simonucci et al 2013;Palmerini et al 2016;Vescovi et al 2019).…”
We analyze the
55
134
Cs
→
56
134
Ba and
55
135
Cs
→
56
135
Ba β
− decays, which are crucial production channels for Ba isotopes in asymptotic giant branch (AGB) stars. We calculate, starting from relativistic quantum mechanics, the effects of multichannel scattering onto weak decays, including nuclear and electronic excited states (ESs) populated above ≃10 keV, for both parent and daughter nuclei. We find increases in the half-lives for T > 108 K (by more than a factor of 3 for 134Cs) as compared to previous works based on systematics. We also discuss our method in view of these previous calculations. An important impact on half-lives comes from nuclear ES decays, while including electronic temperatures yields further increases of about 20% at energies of 10–30 keV, typical of AGB stars of moderate mass (M ≲ 8 M
⊙). Despite properly considering these effects, the new rates remain sensitively lower than the Takahashi & Yokoi values, implying longer half-lives at least above 8–9 keV. Our rate predictions are in substantial accord with recent results based on the shell model, and strongly modify branching ratios along the s-process path previously adopted. With our new rate, nucleosynthesis models well account for the isotopic admixtures of Ba in presolar SiC grains and in the Sun.
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