2021
DOI: 10.48550/arxiv.2112.00772
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$r$-process Nucleosynthesis and Kilonovae from Hypermassive Neutron Star Remnants

Abstract: We investigate 𝑟-process nucleosynthesis and kilonova emission resulting from binary neutron star (BNS) mergers based on a three-dimensional (3D) general-relativistic magnetohydrodynamic (GRMHD) simulation of a hypermassive neutron star (HMNS) remnant. The simulation includes a microphysical finite-temperature equation of state (EOS) and neutrino emission and absorption effects via a leakage scheme. We track the thermodynamic properties of the ejecta using Lagrangian tracer particles and determine its composi… Show more

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Cited by 9 publications
(10 citation statements)
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“…Hot, rapidly spinning PNS-like stars are also generated from the merger of binary neutron stars (e.g., Dessart et al 2009), albeit with higher masses 2M than assumed in our models. However, the limited lifetimes of most such objects before they lose rotational support and collapse into a black hole, may limit the contribution of their neutrino-driven winds relative to other sources of mass ejection during the merger and its aftermath (though strong magnetic fields may change this picture; e.g., Siegel et al 2014;Metzger et al 2018;Curtis et al 2021).…”
Section: Discussionmentioning
confidence: 99%
“…Hot, rapidly spinning PNS-like stars are also generated from the merger of binary neutron stars (e.g., Dessart et al 2009), albeit with higher masses 2M than assumed in our models. However, the limited lifetimes of most such objects before they lose rotational support and collapse into a black hole, may limit the contribution of their neutrino-driven winds relative to other sources of mass ejection during the merger and its aftermath (though strong magnetic fields may change this picture; e.g., Siegel et al 2014;Metzger et al 2018;Curtis et al 2021).…”
Section: Discussionmentioning
confidence: 99%
“…Hot, rapidly spinning PNS-like stars are also generated from the merger of binary neutron stars (e.g., Dessart et al 2009), albeit with higher masses  2 M e than assumed in our models. However, the limited lifetimes of most such objects before they lose rotational support and collapse into a black hole may limit the contribution of their neutrino-driven winds relative to other sources of mass ejection during the merger and its aftermath (though strong magnetic fields may change this picture; e.g., Siegel et al 2014;Metzger et al 2018;Curtis et al 2021).…”
Section: Discussionmentioning
confidence: 99%
“…cases, the mean energies of electron antineutrinos emitted by the disk are 20-50% higher than the mean energies of electron neutrinos, with values becoming close to one another only before a sharp drop at t ∼ 0.5 s. The drop in mean energies is a consequence of energy luminosities decreasing faster with time than number luminosities as the disk transitions to a radiatively inefficient state with lower temperature and density. Due to enhanced neutrino irradiation and suppressed mass loss through the inner boundary, a longer HMNS lifetime correlates with more mass ejected as well as an overall higher average electron fraction and velocity of the unbound ejecta [49,55,56,78,79], which in turn translates into a lower yield of heavy r-process elements [51,80,81] (Table I). Our model t010-ab00 has a slightly lower average Y e than the prompt BH model due to a relative increase in the ejecta with Y e < 0.25 material (Figure 2)…”
Section: Mass In Bin [M ]mentioning
confidence: 99%