TY - JOUR
T1 - The impact of r-process heating on the dynamics of neutron star merger accretion disc winds and their electromagnetic radiation
AU - Klion, Hannah
AU - Tchekhovskoy, Alexander
AU - Kasen, Daniel
AU - Kathirgamaraju, Adithan
AU - Quataert, Eliot
AU - Fernández, Rodrigo
N1 - Funding Information:
This research was funded by the Gordon and Betty Moore Foundation through grant GBMF5076. AT was supported by NASA 80NSSC18K0565 and NSF AST-1815304 grants. EQ was supported in part by a Simons Investigator award from the Simons Foundation. RF acknowledges support from the Natural Sciences and Engi- neering Research Council (NSERC) of Canada through Disco v ery Grant RGPIN-2017-04286, and from the Faculty of Science at the University of Alberta. The simulations presented here were carried out and processed using the National Energy Research Scientific Computing Center, a U.S. Department of Energy Office of Science User Facility, and the Savio computational cluster resource provided by the Berkeley Research Computing program at the University of California, Berkeley (supported by the UC Berkeley Chancellor, Vice Chancellor of Research, and Office of the CIO).
Publisher Copyright:
© 2022 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society.
PY - 2022/2
Y1 - 2022/2
N2 - Neutron star merger accretion discs can launch neutron-rich winds of >10-2M⊙. This ejecta is a prime site for r-process nucleosynthesis, which will produce a range of radioactive heavy nuclei. The decay of these nuclei releases enough energy to accelerate portions of the wind by ∼0.1c. Here, we investigate the effect of r-process heating on the dynamical evolution of disc winds. We extract the wind from a 3D general relativistic magnetohydrodynamic simulation of a disc from a post-merger system. This is used to create inner boundary conditions for 2D hydrodynamic simulations that continue the original 3D simulation. We perform two such simulations: one that includes the r-process heating, and another one that does not. We follow the hydrodynamic simulations until the winds reach homology (60 s). Using time-dependent multifrequency multidimensional Monte Carlo radiation transport simulations, we then calculate the kilonova light curves from the winds with and without dynamical r-process heating. We find that the r-process heating can substantially alter the velocity distribution of the wind, shifting the mass-weighted median velocity from 0.06c to 0.12c. The inclusion of the dynamical r-process heating makes the light curve brighter and bluer at $\sim 1\, \mathrm{d}$ post-merger. However, the high-velocity tail of the ejecta distribution and the early ($\lesssim 1\, \mathrm{d}$) light curves are largely unaffected.
AB - Neutron star merger accretion discs can launch neutron-rich winds of >10-2M⊙. This ejecta is a prime site for r-process nucleosynthesis, which will produce a range of radioactive heavy nuclei. The decay of these nuclei releases enough energy to accelerate portions of the wind by ∼0.1c. Here, we investigate the effect of r-process heating on the dynamical evolution of disc winds. We extract the wind from a 3D general relativistic magnetohydrodynamic simulation of a disc from a post-merger system. This is used to create inner boundary conditions for 2D hydrodynamic simulations that continue the original 3D simulation. We perform two such simulations: one that includes the r-process heating, and another one that does not. We follow the hydrodynamic simulations until the winds reach homology (60 s). Using time-dependent multifrequency multidimensional Monte Carlo radiation transport simulations, we then calculate the kilonova light curves from the winds with and without dynamical r-process heating. We find that the r-process heating can substantially alter the velocity distribution of the wind, shifting the mass-weighted median velocity from 0.06c to 0.12c. The inclusion of the dynamical r-process heating makes the light curve brighter and bluer at $\sim 1\, \mathrm{d}$ post-merger. However, the high-velocity tail of the ejecta distribution and the early ($\lesssim 1\, \mathrm{d}$) light curves are largely unaffected.
KW - neutron star mergers
KW - radiative transfer
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U2 - 10.1093/mnras/stab3583
DO - 10.1093/mnras/stab3583
M3 - Article
AN - SCOPUS:85126454388
SN - 0035-8711
VL - 510
SP - 2968
EP - 2979
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 2
ER -