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r-Process Nucleosynthesis With Ab Initio Nuclear Masses Around The N=82 Shell Closure

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arxiv 2509.19131 v2 pith:HF7FLXFN submitted 2025-09-23 astro-ph.HE nucl-exnucl-th

r-Process Nucleosynthesis With Ab Initio Nuclear Masses Around The N=82 Shell Closure

classification astro-ph.HE nucl-exnucl-th
keywords r-processinitiomassespeakaroundbeyondclosuremass
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Our understanding of the origin of heavy elements beyond iron relies on the rapid neutron capture process (r-process), which accounts for roughly half of their cosmic abundance. However, the extreme neutron-rich conditions required for the r-process involve many nuclei that remain experimentally inaccessible, making theoretical predictions essential. We explore the impact of nuclear masses calculated with the ab initio valence-space in-medium similarity renormalization group, focusing on the region around the N = 82 shell closure. We show for the first time that such ab initio mass calculations can be used to refine r-process predictions compared to global, but more phenomenological mass models. With the ab initio masses, the waiting point of the second r-process peak is strengthened, which leads to an overall slower nucleosynthesis flow, lower abundances of nuclei beyond the peak, and a stronger shift of the third r-process peak.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. High-order perturbative calculations of nuclear ground states: Automated evaluation of many-body diagrams

    nucl-th 2026-06 unverdicted novelty 7.0

    Automated MBPT up to fifth order shows convergence trends in ground-state energies of closed-shell nuclei and decomposes fourth-order terms while comparing to IMSRG.

  2. Computational schemes for the Magnus expansion of the in-medium similarity renormalization group

    nucl-th 2026-01 unverdicted novelty 4.0

    The hunter-gatherer scheme for the Magnus expansion in IMSRG(3) approximations introduces differences of up to 7 MeV in ground-state energies and 0.5 MeV in excitation energies compared to standard IMSRG(2) methods.