TY - JOUR
T1 - Properties of Kilonovae from Dynamical and Post-merger Ejecta of Neutron Star Mergers
AU - Tanaka, Masaomi
AU - Kato, Daiji
AU - Gaigalas, Gediminas
AU - Rynkun, Pavel
AU - Radžiute, Laima
AU - Wanajo, Shinya
AU - Sekiguchi, Yuichiro
AU - Nakamura, Nobuyuki
AU - Tanuma, Hajime
AU - Murakami, Izumi
AU - Sakaue, Hiroyuki A.
N1 - Funding Information:
We thank Kenta Hotokezaka, Masaru Shibata, Nobuya Nishimura, Kenta Kiuchi, and Koutarou Kyutoku for providing results of simulations and fruitful discussion, and the anonymous referee for constructive comments. M.T. thanks the Institute for Nuclear Theory (INT) at the University of Washington for its hospitality and the Department of Energy for partial support during the completion of this work. M.T. also thanks Rodrigo Fernández, Brian Metzger, Daniel Kasen, and Gabriel Martinez-Pinedo for organizing the workshop and providing the nice research environment at INT. Numerical simulations presented in this paper were carried out with Cray XC30 at the Center for Computational Astrophysics, National Astronomical Observatory of Japan. Computations by G.G. were performed on resources at the High Performance Computing Center “HPC Sauletekis” of the Faculty of Physics at Vilnius University. This research was supported by the NINS program for cross-disciplinary science study, the Inoue Science Research Award from Inoue Foundation for Science, the RIKEN iTHES project, a post-K computer project (Priority issue No. 9) of MEXT, and Grants-in-Aid for Scientific Research from JSPS (15H00782, 15H02075, 15K05077, 16H02183, 16H06341, 16K17706, 17K05391, 26400237) and MEXT (17H06357, 17H06363).
Publisher Copyright:
© 2018. The American Astronomical Society. All rights reserved.
PY - 2018/1/10
Y1 - 2018/1/10
N2 - Ejected material from neutron star mergers gives rise to electromagnetic emission powered by radioactive decays of r-process nuclei, the so-called kilonova or macronova. While properties of the emission are largely affected by opacities in the ejected material, available atomic data for r-process elements are still limited. We perform atomic structure calculations for r-process elements: Se (Z = 34), Ru (Z = 44), Te (Z = 52), Ba (Z = 56), Nd (Z = 60), and Er (Z = 68). We confirm that the opacities from bound-bound transitions of open f-shell, lanthanide elements (Nd and Er) are higher than those of the other elements over a wide wavelength range. The opacities of open s-shell (Ba), p-shell (Se and Te), and d-shell (Ru) elements are lower than those of open f-shell elements, and their transitions are concentrated in the ultraviolet and optical wavelengths. We show that the optical brightness can be different by mag depending on the element abundances in the ejecta such that post-merger, lanthanide-free ejecta produce brighter and bluer optical emission. Such blue emission from post-merger ejecta can be observed from the polar directions if the mass of the preceding dynamical ejecta in these regions is small. For the ejecta mass of 0.01 M⊙, observed magnitudes of the blue emission will reach 21.0 mag (100 Mpc) and 22.5 mag (200 Mpc) in the g and r bands within a few days after the merger, which are detectable with 1 m or 2 m class telescopes.
AB - Ejected material from neutron star mergers gives rise to electromagnetic emission powered by radioactive decays of r-process nuclei, the so-called kilonova or macronova. While properties of the emission are largely affected by opacities in the ejected material, available atomic data for r-process elements are still limited. We perform atomic structure calculations for r-process elements: Se (Z = 34), Ru (Z = 44), Te (Z = 52), Ba (Z = 56), Nd (Z = 60), and Er (Z = 68). We confirm that the opacities from bound-bound transitions of open f-shell, lanthanide elements (Nd and Er) are higher than those of the other elements over a wide wavelength range. The opacities of open s-shell (Ba), p-shell (Se and Te), and d-shell (Ru) elements are lower than those of open f-shell elements, and their transitions are concentrated in the ultraviolet and optical wavelengths. We show that the optical brightness can be different by mag depending on the element abundances in the ejecta such that post-merger, lanthanide-free ejecta produce brighter and bluer optical emission. Such blue emission from post-merger ejecta can be observed from the polar directions if the mass of the preceding dynamical ejecta in these regions is small. For the ejecta mass of 0.01 M⊙, observed magnitudes of the blue emission will reach 21.0 mag (100 Mpc) and 22.5 mag (200 Mpc) in the g and r bands within a few days after the merger, which are detectable with 1 m or 2 m class telescopes.
KW - gravitational waves
KW - nuclear reactions, nucleosynthesis, abundances
KW - opacity
KW - radiative transfer
KW - stars: neutron
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U2 - 10.3847/1538-4357/aaa0cb
DO - 10.3847/1538-4357/aaa0cb
M3 - Article
AN - SCOPUS:85040693998
SN - 0004-637X
VL - 852
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 2
M1 - 109
ER -