2022ApJ...931L..23L


Query : 2022ApJ...931L..23L

2022ApJ...931L..23L - Astrophys. J., 931, L23-L23 (2022/June-1)

GRB 211227A as a Peculiar Long Gamma-Ray Burst from a Compact Star Merger.

LU H.-J., YUAN H.-Y., YI T.-F., WANG X.-G., HU Y.-D., YUAN Y., RICE J., WANG J.-G., CAO J.-X., KONG D.-F., FERNANDEZ-GARCIA E., CASTRO-TIRADO A.J., LIAN J.-S., GAN W.-P., WANG S.-Q., XIN L.-P., CABALLERO-GARCIA M.D., FAN Y.-F. and LIANG E.-W.

Abstract (from CDS):

Long-duration gamma-ray bursts (GRBs) associated with supernovae (SNe) are believed to originate from massive star core-collapse events, whereas short-duration GRBs that are related to compact star mergers are expected to be accompanied by kilonovae. GRB 211227A, which lasted about 84 s, had an initial short/hard spike followed by a series of soft gamma-ray extended emission at redshift z = 0.228. We performed follow-up observations of the optical emission using BOOTES, LCOGT, and the Lijiang 2.4 m telescope, but we detected no associated supernova signature, even down to very stringent limits at such a low redshift. We observed the host galaxy within a large error circle and roughly estimated the physical offset of GRB 211227A as 20.47 ± 14.47 kpc from the galaxy center. These properties are similar to those of GRB 060614, and suggest that the progenitor of GRB 211227A is not favored to be associated with the death of massive stars. Hence, we propose that GRB 211227A originates from a compact star merger. Calculating pseudo-kilonova emission for this case by adopting the typical parameters, we find that any associated pseudo-kilonova is too faint to be detected. If this is the case, it explains naturally the characteristics of the prompt emission, the lack of SN and kilonova emission, and the large physical offset from the galaxy center.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gamma-ray bursts

Simbad objects: 21

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Number of rows : 21
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 GRB 200826A gB 00 27 08.47 +34 01 36.5           ~ 121 0
2 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
3 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
4 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 140 0
5 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
6 GRB 051227 gB 08 20 58.107 +31 55 32.01           ~ 127 0
7 GRB 211227A gB 08 48 35.73 -02 44 07.1           ~ 57 0
8 UCAC4 217-047923 * 10 19 02.5992684123 -46 40 11.294771086   13.795 12.458 12.114   ~ 54 0
9 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
10 GRB 011121 gB 11 34 26.67 -76 01 41.6       23.0   ~ 286 1
11 GALEX J123205.0-105600 Bz? 12 32 04.9717245480 -10 56 00.722548932         16.421 ~ 186 0
12 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
13 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
14 SN 2013dx SN* 14 29 14.77 +15 46 26.6           ~ 178 0
15 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
16 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
17 GRB 080503 gB 19 06 28.74 +68 47 35.8           ~ 172 0
18 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
19 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
20 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 138 0
21 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1

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