2024A&A...690L...9M


Query : 2024A&A...690L...9M

2024A&A...690L...9M - Astronomy and Astrophysics, volume 690L9 (2024/10-1)

Disk mass after a binary neutron star merger as a constraining parameter for short gamma-ray bursts.

MPISKETZIS V. and NATHANAIL A.

Abstract (from CDS):

Context. The coincident detection of GW170817 and gamma-ray burst GRB170817A marked a milestone for the connection between binary neutron star (BNS) mergers and short gamma-ray bursts (sGRBs). These mergers can lead to the formation of a black hole that is surrounded by a disk and to the generation of a powerful jet. It spends energy to break free from the merger ejecta, and then a portion of it is dissipated to produce observable emissions.
Aims. Our primary goal is to enhance our comprehension of BNS mergers by constraining the disk mass for a selection of sGRBs. To do this, we used the isotropic gamma-ray luminosity and corresponding emission times as key indicators.
Methods. We leveraged data from GW170817 to estimate the disk mass surrounding the BNS merger remnant, and we subsequently inferred the efficiency of the accretion onto the jet. We then statistically examined other sGRB observations to estimate whether they might have been induced by BNS mergers
Results. Our findings suggest that when similar physical parameters are employed as in the only observed BNS-powered GRB event, GRB170817A, a substantial fraction of sGRBs would need an unrealistically massive disk remnant.
Conclusions. This observation raises the possibility that either a different mechanism powered those events or that the post-collapse disk efficiency varies significantly in different BNS merger scenarios.

Abstract Copyright: © The Authors 2024

Journal keyword(s): stars: black holes - gamma-ray burst: general - stars: neutron

Simbad objects: 28

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Number of rows : 28
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 Fermi bn150120123 G 00 41 16.5630 +33 59 42.598           ~ 70 0
3 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
4 GRB 141212A G 02 36 29.9570 +18 08 47.228           ~ 70 0
5 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
6 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
7 GRB 061217 gB 10 41 39.320 -21 07 22.11           ~ 128 0
8 GRB 201221D gB 11 24 14.19 +42 08 35.5           ~ 48 0
9 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
10 GALEX J123205.0-105600 Bz? 12 32 04.9717245480 -10 56 00.722548932         16.421 ~ 186 0
11 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
12 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
13 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
14 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
15 SDSS J140910.47+275320.8 G 14 09 10.47535 +27 53 20.8393           ~ 279 0
16 GRB 150423A gB 14 46 18.96 +12 17 00.6           ~ 79 0
17 GRB 140903A G 15 52 03.2650 +27 36 10.710           ~ 138 0
18 GRB 050813 gB 16 07 57.190 +11 14 57.80           ~ 147 0
19 GRB 190627A gB 16 19 18.73 -05 17 20.4           ~ 43 0
20 GRB 060502B gB 18 35 46.060 +52 37 51.45           ~ 153 1
21 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
22 Fermi bn131004904 gB 19 44 27.20 -02 57 31.0           ~ 113 0
23 GRB 140622A gB 21 08 41.56 -14 25 09.5           ~ 61 0
24 GRB 070429B G 21 52 03.6910 -38 49 42.820           ~ 125 0
25 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
26 Fermi bn160624477 gB 22 00 46.21 +29 38 37.8           ~ 69 0
27 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
28 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0

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