2024ApJ...964..195M


Query : 2024ApJ...964..195M

2024ApJ...964..195M - Astrophys. J., 964, 195 (2024/April-1)

Contribution of γ-Ray Burst Afterglow Emissions to the Isotropic Diffuse γ-Ray Background.

MIN F.-S., YAO Y.-H., LIU R.-Y., CHEN S., LU H. and GUO Y.-Q.

Abstract (from CDS):

The isotropic diffuse γ-ray background (IGRB) serves as a fundamental probe of the evolution of the extreme Universe. Although various astrophysical sources have been proposed as potential contributors to the IGRB, the dominant population is still under debate. γ-ray bursts (GRBs) are among candidate contributors of IGRB, although they are not as frequently discussed as blazars or starburst galaxies. Recent observations of TeV emission from GRB afterglows have provided fresh insights into this subject. This work aims to investigate the potential contribution of GRB afterglows to the IGRB under the standard afterglow model. We carefully examine the influence of each microphysical parameter of the afterglow model on this contribution, with a particular emphasis on the significant role played by the initial kinematic energy. To determine the energy and quantify the contribution of GRB afterglow to IGRBs, we utilize the observed GRB afterglow energy emissions from the Swift X-ray Telescope and Fermi Large Area Telescope instruments. Our calculations, considering the synchrotron self-Compton emission, suggest that GRB afterglows make up less than 10% of the IGRBs. To enhance the precision of our findings, it is crucial to further constrain these parameters by conducting additional ground-based observations of GRB afterglows.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gamma-ray bursts

Simbad objects: 33

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Number of rows : 33
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 180720B gB 00 02 06.99 -02 55 07.8           ~ 215 0
2 GRB 220101A gB 00 05 24.89 +31 46 07.7           ~ 85 0
3 GRB 201104B gB 00 20 51.46 +07 50 30.7           ~ 21 0
4 Fermi bn131231198 gB 00 42 44.0 -01 29 40           ~ 103 0
5 GRB 201021C gB 00 50 06.93 -55 51 55.8           ~ 21 0
6 GRB 201014A gB 01 23 11.09 +27 39 36.9           ~ 18 0
7 GRB 221110A gB 01 56 23.81 -27 17 44.5           ~ 15 0
8 SN 2019oyw SN* 02 58 10.510 -08 57 27.20           ~ 218 0
9 GRB 191011A gB 02 58 54.70 -27 50 43.4           ~ 38 0
10 GRB 191004B gB 03 16 48.97 -39 38 06.3           ~ 32 0
11 GRB 181010A gB 03 30 16.88 -23 02 17.9           ~ 39 0
12 GRB 190114C gB 03 38 01.18 -26 56 47.8           ~ 343 0
13 GRB 171010A gB 04 26 19.41 -10 27 47.9           SNIc-BL 109 0
14 GRB 090328 gB 06 02 39.69 -41 52 55.1           ~ 194 1
15 Fermi bn120711115 gB 06 18 42.839 -70 59 56.78           ~ 125 0
16 GRB 230116D gB 06 34 28.28 +49 52 22.3           ~ 21 0
17 Fermi bn150314205 gB 08 26 40.82 +63 50 03.4           ~ 117 0
18 GRB 211207A gB 09 58 29.69 -24 21 32.2           ~ 11 0
19 GRB 191221B gB 10 19 19.17 -38 09 27.5           ~ 66 0
20 GRB 210702A gB 11 14 18.89 -36 44 49.8           ~ 40 0
21 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
22 Fermi bn090323002 gB 12 42 50.28 +17 03 11.9           ~ 244 1
23 GRB 221009A gB 19 13 03.85 +19 46 22.7           ~ 433 0
24 GRB 210411C gB 19 46 26.74 -39 23 53.4           ~ 21 0
25 GRB 230325A gB 19 47 23.94 -46 04 33.9           ~ 15 0
26 GRB 210731A gB 20 01 13.13 -28 03 39.7           ~ 28 0
27 GRB 210822A gB 20 17 44.99 +05 17 00.5           ~ 49 0
28 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
29 GRB 210905A gB 20 36 11.64 -44 26 24.3           ~ 42 0
30 Fermi bn160509374 gB 20 47 00.90 +76 06 30.1           ~ 141 0
31 GRB 210619B gB 21 18 52.39 +33 51 00.2           ~ 93 0
32 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0
33 GRB 210517A gB 23 52 53.81 -39 06 06.7           ~ 13 0

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