2020ApJ...903L...3W


Query : 2020ApJ...903L...3W

2020ApJ...903L...3W - Astrophys. J., 903, L3-L3 (2020/November-1)

MeV gamma rays from fission: a distinct signature of actinide production in Neutron star mergers.

WANG X., VASSH N., SPROUSE T., MUMPOWER M., VOGT R., RANDRUP J. and SURMAN R.

Abstract (from CDS):

Neutron star mergers (NSMs) are the first verified sites of rapid neutron capture (r-process) nucleosynthesis, and could emit gamma rays from the radioactive isotopes synthesized in the neutron-rich ejecta. These MeV gamma rays may provide a unique and direct probe of the NSM environment as well as insight into the nature of the r process, just as observed gammas from the 56Ni radioactive decay chain provide a window into supernova nucleosynthesis. In this work, we include the photons from fission processes for the first time in estimates of the MeV gamma-ray signal expected from an NSM event. We consider NSM ejecta compositions with a range of neutron richness and find a dramatic difference in the predicted signal depending on whether or not fissioning nuclei are produced. The difference is most striking at photon energies above ∼3.5 MeV and at a relatively late time, several days after the merger event, when the ejecta is optically thin. We estimate that a Galactic NSM could be detectable by a next generation gamma-ray detector such as AMEGO in the MeV range, up to ∼104 days after the merger, if fissioning nuclei are robustly produced in the event.

Abstract Copyright: © 2020. The American Astronomical Society. All rights reserved.

Journal keyword(s): R-process - Nucleosynthesis - Compact binary stars - Gamma-rays - Gamma-ray transient sources - Supernovae

Simbad objects: 3

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Number of rows : 3
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 SN 1987A SN* 05 35 27.98840 -69 16 11.1134           SNIIpec 5203 2
2 SN 2014J SN* 09 55 42.12 +69 40 25.9           SNIa-norm 456 1
3 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0

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