Uncertainties in the nu p-process: supernova dynamics versus nuclear physics

TL;DR

This study investigates how supernova dynamics and nuclear physics uncertainties influence the nu p-process, revealing key factors like wind termination, electron fraction, and nuclear reaction rates that affect p-nuclei production.

Contribution

It provides a detailed analysis of the effects of supernova wind termination and nuclear data uncertainties on the nu p-process, highlighting critical parameters for p-nuclei synthesis.

Findings

Wind termination within 1.5-3 billion K enhances nu p-process efficiency.

Y_{e,3} values of 0.52-0.60 produce p-nuclei up to A=108.

Variations in nuclear reaction rates significantly impact p-nuclei yields.

Abstract

We examine how the uncertainties involved in supernova dynamics as well as in nuclear data inputs affect the nup-process in the neutrino-driven winds. For the supernova dynamics, we find that the wind termination by the preceding dense ejecta shell, as well as the electron fraction (Y_{e, 3}; at 3 10^9 K) play a crucial role. A wind termination within the temperature range of (1.5-3) 10^9 K greatly enhances the efficiency of the nu p-process. This implies that the early wind phase, when the innermost layer of the preceding supernova ejecta is still 200-1000 km from the center, is most relevant to the nup-process. The outflows with Y_{e, 3} = 0.52-0.60 result in the production of the p-nuclei up to A=108 with interesting amounts. Furthermore, the p-nuclei up to A=152 can be produced if Y_{e, 3} = 0.65 is achieved. For the nuclear data inputs, we test the sensitivity to the rates relevant to the breakout from the pp-chain region (A < 12), to the (n, p) rates on heavy nuclei, and to the nuclear masses along the nup-process pathway. We find that a small variation of the rates of triple-alpha and of the (n, p) reaction on 56Ni leads to a substantial change in the p-nuclei production. We also find that 96Pd (N=50) on the nup-process path plays a role as a second seed nucleus for the production of heavier p-nuclei. The uncertainty in the nuclear mass of 82Zr can lead to a factor of two reduction in the abundance of the p-isotope 84Sr.