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    Fission and the r-process nucleosynthesis of translead nuclei in neutron star mergers

    Samuel A. Giuliani1,*, Gabriel Martínez-Pinedo2,3,4,†, Meng-Ru Wu5,6,7,‡, and Luis M. Robledo8,9,§

    • 1Department of Physics and Astronomy and NSCL/FRIB Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
    • 2GSI Helmholtzzentrum für Schwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany
    • 3Institut für Kernphysik (Theoriezentrum), Department of Physics, Technische Universität Darmstadt, Schlossgartenstraße 2, 64298 Darmstadt, Germany
    • 4Helmholtz Forschungsakademie Hessen für FAIR, GSI Helmholtzzentrum für Schwerionenforschung, Planckstraße 1, 64291 Darmstadt, Germany
    • 5Institute of Physics, Academia Sinica, Taipei, 11529, Taiwan
    • 6Institute of Astronomy and Astrophysics, Academia Sinica, Taipei 10617, Taiwan
    • 7Physics Division, National Center for Theoretical Sciences, 30013 Hsinchu, Taiwan
    • 8Center for Computational Simulation, Universidad Politécnica de Madrid, Campus de Montegancedo, 28660 Madrid, Spain
    • 9Departamento de Física Teórica and CIAFF, Universidad Autónoma de Madrid, 28049 Madrid, Spain

    • *giuliani@nscl.msu.edu
    • †g.martinez@gsi.de
    • ‡mwu@gate.sinica.edu.tw
    • §luis.robledo@uam.es

    Phys. Rev. C 102, 045804 – Published 9 October, 2020

    DOI: https://doi.org/10.1103/PhysRevC.102.045804

    Abstract

    We study the impact of fission on the production and destruction of translead nuclei during the r-process nucleosynthesis occurring in neutron-star mergers. Abundance patterns and rates of nuclear energy production are obtained for different ejecta conditions using three sets of stellar reaction rates, one of which is based on microscopic and consistent calculations of nuclear masses, fission barriers, and collective inertias. We show that the accumulation of fissioning material during the r process can strongly affect the free neutron abundance after the r-process freeze-out. This leads to a significant impact on the abundances of heavy nuclei that undergo α decay or spontaneous fission, affecting the radioactive energy production by the ejecta at timescales relevant for kilonova emission.

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