2023ApJ...949L..22D


Query : 2023ApJ...949L..22D

2023ApJ...949L..22D - Astrophys. J., 949, L22 (2023/June-1)

Evidence for Two Distinct Populations of Kilonova-associated Gamma-Ray Bursts.

DIMPLE, MISRA K. and ARUN K.G.

Abstract (from CDS):

Identification of gamma-ray burst (GRB) progenitors based on the duration of their prompt emission (T90) has faced several roadblocks recently. Long-duration GRBs (with T90 > 2 s) have traditionally been thought to be originating from the collapse of massive stars and the short-duration ones (with T90 < 2 s) from compact binary mergers. However, recent observations of a long GRB associated with a kilonova (KN) and a short GRB with supernova association demand a more detailed classification of the GRB population. In this Letter, we focus on GRBs associated with KNe, believed to be originating from mergers of binaries involving neutron stars (NSs). We make use of the GRB prompt-emission light curves of the Swift/BAT 2022 GRB catalog and employ machine-learning algorithms to study the classification of GRB progenitors. Our analysis reveals that there are five distinct clusters of GRBs, of which the KN-associated GRBs are located in two separate clusters, indicating they may have been produced by different progenitors. We argue that these clusters may be due to subclasses of binary neutron star and/or NS-black hole mergers. We also discuss the implications of these findings for future gravitational-wave observations and how those observations may help in understanding these clusters better.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gamma-ray bursts - Gamma-ray transient sources

Simbad objects: 25

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Number of rows : 25
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 SDSS J002243.71-001657.5 G 00 22 43.71720 -00 16 57.5256           ~ 69 0
2 GRB 200826A gB 00 27 08.47 +34 01 36.5           ~ 121 0
3 Fermi bn120729456 gB 00 52 17.84 +49 56 23.1           ~ 122 0
4 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
5 GRB 071112C gB 02 36 50.89 +28 22 16.9           ~ 164 0
6 SN 2013ez SN* 02 53 56.70 +13 23 13.6           ~ 118 0
7 SN 2019oyw SN* 02 58 10.510 -08 57 27.20           ~ 218 0
8 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
9 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
10 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
11 GRB 171010A gB 04 26 19.41 -10 27 47.9           SNIc-BL 109 0
12 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 140 0
13 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 336 1
14 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
15 GRB 211227A gB 08 48 35.73 -02 44 07.1           ~ 57 0
16 Fermi bn111228657 gB 10 00 16.04 +18 17 52.2           ~ 201 0
17 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
18 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
19 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
20 SDSS J140910.47+275320.8 G 14 09 10.47535 +27 53 20.8393           ~ 279 0
21 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
22 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
23 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 286 1
24 SN 2012eb SN* 23 41 38.35 -46 11 07.0           SNIb/c 62 1
25 SN 2013fu SN* 23 54 29.91 +29 25 47.6           SNIb/c 144 1

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