2025MNRAS.542.2857W


Query : 2025MNRAS.542.2857W

2025MNRAS.542.2857W - Mon. Not. R. Astron. Soc., 542, 2857-2865 (2025/October-1)

The colour evolution of magnetar-powered kilonova emission in merging neutron star-neutron star systems.

WANG S.-N., LU H.-J., LIU X.-X., RICE J., REN J. and LIANG E.-W.

Abstract (from CDS):

The first direct detection of the gravitational wave (GW) event GW170817 and its electromagnetic (EM) counterpart open a new window for studying of multimessenger astronomy. However, how to identify the remnant of binary neutron star (NS) merger via EM radiation remain an open question. In this paper, we propose a method of colour evolution of kilonova emission to identify its progenitors. We assume that the energy of the kilonova is contributed from radioactive decay, magnetar spin-down, and pulsar wind nebula (PWN). The colour evolution of kilonova emission associated with short GRB is significant when the spectrum is thermal emission, while it tends towards a constant when the spectrum is non-thermal radiation. On the other hand, if the central engine is a black hole (BH) which is promptly generated by the NS-NS merger or NS-BH merger, then the kilonova is powered only by the radioactive decay. There is no colour evolution at the beginning before the peak of kilonova emission, but is significantly and rapidly increasing after the peak. On the contrary, if the central engine is a magnetar or stable NS, the kilonova emission is contributed from radioactive decay, magnetar, and PWN. The colour evolution after the peak of kilonova emission is complex behaviour which depends on the rotational energy and spin-down time-scale of magnetar, and finally tend to a constant in the late state.

Abstract Copyright: © The Author(s) 2025. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): neutron star mergers

Simbad objects: 5

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Number of rows : 5
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 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
2 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
3 GrW 230529 181500 GWE ~ ~           ~ 45 0
4 GrW 200105 GWE ~ ~           ~ 136 0
5 GrW 200115 GWE ~ ~           ~ 160 0

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