• DOI:10.1093/mnras/stw2622
• Corpus ID: 41139994

The influence of neutrinos on r-process nucleosynthesis in the ejecta of black hole-neutron star mergers

@article{Roberts2017TheIO,
  title={The influence of neutrinos on r-process nucleosynthesis in the ejecta of black hole-neutron star mergers},
  author={Luke F Roberts and Jonas Lippuner and Matthew D Duez and Joshua A. Faber and Francois Foucart and James C. Lombardi and Sandra Ning and Christian D. Ott and Marcelo Ponce},
  journal={Monthly Notices of the Royal Astronomical Society},
  year={2017},
  volume={464},
  pages={3907-3919}
}

• L. Roberts, J. Lippuner, +6 authors M. Ponce
• Published 28 January 2016
• Physics
• Monthly Notices of the Royal Astronomical Society

During the merger of a black hole and a neutron star, baryonic mass can become unbound from the system. Because the ejected material is extremely neutron-rich, the r-process rapidly synthesizes heavy nuclides as the material expands and cools. In this work, we map general relativistic models of black hole–neutron star mergers into a Newtonian smoothed particle hydrodynamics (SPH) code and follow the evolution of the thermodynamics and morphology of the ejecta until the outflows become homologous. We investigate how the subsequent evolution depends on our mapping procedure and find that the results are robust. Using thermodynamic histories from the SPH particles, we then calculate the expected nucleosynthesis in these outflows while varying the level of neutrino irradiation coming from the post-merger accretion disc. We find that the ejected material robustly produces r-process nucleosynthesis even for unrealistically high neutrino luminosities, due to the rapid velocities of the outflow. None the less, we find that neutrinos can have an impact on the detailed pattern of the r-process nucleosynthesis. Electron neutrinos are captured by neutrons to produce protons while neutron capture is occurring. The produced protons rapidly form low-mass seed nuclei for the r-process. These low-mass seeds are eventually incorporated into the first r-process peak at A ∼ 78. We consider the mechanism of this process in detail and discuss if it can impact galactic chemical evolution of the first peak r-process nuclei.