Abstract

ABSTRACT The origin of the proton-rich trans-iron isotopes in the Solar system is still uncertain. Single-degenerate thermonuclear supernovae (SNIa) with n-capture nucleosynthesis seeds assembled in the external layers of the progenitor’s rapidly accreting white dwarf (RAWD) phase may produce these isotopes. We calculate the stellar structure of the accretion phase of five white dwarf (WD) models with initial masses ≥ 0.85 $\, \mathrm{M}_\odot$ using the stellar code mesa The near-surface layers of the 1, 1.26, 1.32 and 1.38 $\, \mathrm{M}_\odot$ models are most representative of the regions in which the bulk of the p nuclei are produced during SNIa explosions, and for these models we also calculate the neutron-capture nucleosynthesis in the external layers. Contrary to previous RAWD models at lower mass, we find that the H-shell flashes are the main site of n-capture nucleosynthesis. We find high neutron densities up to several 1015 cm−3 in the most massive WDs. Through the recurrence of the H-shell flashes these intermediate neutron densities can be sustained effectively for a long time leading to high-neutron exposures with a strong production up to Pb. Both the neutron density and the neutron exposure increase with increasing the mass of the accreting WD. Finally, the SNIa nucleosynthesis is calculated using the obtained abundances as seeds. We obtain solar to supersolar abundances for p-nuclei with A > 96. Our models show that SNIa are a viable p-process production site.

Highlights

  • At the end of the asymptotic giant branch (AGB) evolution, low mass and massive AGB stars (M < 8 M ) loose all their envelope, and cool down as carbon–oxygen (CO) white dwarfs (WDs) (e.g. Herwig 2005; Karakas & Lattanzio 2014)

  • We calculate the stellar structure of the accretion phase of five white dwarf (WD) models with initial masses ≥ 0.85 M using the stellar code MESA The near-surface layers of the 1, 1.26, 1.32 and 1.38 M models are most representative of the regions in which the bulk of the p nuclei are produced during SNIa explosions, and for these models we calculate the neutron-capture nucleosynthesis in the external layers

  • Contrary to previous rapidly accreting white dwarf (RAWD) models at lower mass, we find that the H-shell flashes are the main site of n-capture nucleosynthesis

Read more

Summary

INTRODUCTION

At the end of the asymptotic giant branch (AGB) evolution, low mass and massive AGB stars (M < 8 M ) loose all their envelope, and cool down as carbon–oxygen (CO) white dwarfs (WDs) (e.g. Herwig 2005; Karakas & Lattanzio 2014). The H ingestion in the relatively low-mass WDs simulated by Denissenkov et al (2017) do not show the split of the convection zone and can maintain the H-ingestion conditions and the associated high neutron density for many month, thereby creating the conditions for heavy-element production in RAWDs. Denissenkov et al (2019) presented i-process yields for seven metallicities from solar to [Fe/H] = −2.6 and showed that low-metallicity RAWD models can naturally explain the observed abundance of most CEMP-r/s stars. This effect has been found at metallicities equal or larger than Z = 0.01, while a contribution from lower metallicities, essential to boost the Galactic γ -process contribution of massive stars, is currently under investigation For this reason, it is essential to consider a complementary p-process source that could be represented by SNIa. In this work, we will present our simulations of WDs accreting solar-composition matter.

ACCRETING WD MODELS
Identification of different burning regimes
Accretion models
H-ingestion events in WD-accretion models
Building the seeds for the p-process
SNIa nucleosynthesis calculation
Findings
SUMMARY AND CONCLUSIONS

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.