2020ApJ...894...11G


Query : 2020ApJ...894...11G

2020ApJ...894...11G - Astrophys. J., 894, 11-11 (2020/May-1)

The luminosity distribution of short gamma-ray bursts under a structured jet scenario.

GUO Q., WEI D. and WANG Y.

Abstract (from CDS):

The joint detection of gravitational wave (GW) and electromagnetic radiation from the binary neutron star merger event GW170817 marks a breakthrough in the field of multi-messenger astronomy. The short gamma-ray burst (sGRB) GRB 170817A, associated with this binary neutron star merger event, has an isotropic-equivalent gamma-ray radiation luminosity of 1.6 x 1047 erg s–1, which is much lower than that of other sGRBs. The measurement of the superluminal movement of the radio afterglow emission confirms the presence of the relativistic jet, and the emission features can be well explained by the structured jet model. In this paper, we calculate the luminosity distribution of sGRBs and its evolution with redshift based on the structured (Gaussian) jet model, and find that the typical luminosity increase with redshift, for nearby sGRBs (such as for luminosity distance less than 200 Mpc) the typical gamma-ray luminosity is just around 1047-1048 erg s–1, which naturally explains the very low radiation luminosity of GRB 170817A. We derived the detection probability of sGRBs by Fermi-GBM and found that the expected detection rate of sGRBs is only about 1 yr–1 within the distance of several hundred Mpc. We explored the effect of the power-law index α of the merger time distribution on the observed characteristics and found that it had little effect on the observed luminosity and viewing-angle distributions. However, it is very interesting that, for different values of α, the distributions of the number of observed sGRBs are quite different, so it is possible to determine the value of α through observed distributions of the number of sGRBs. We used the Bayesian method to make a quantitative analysis and found that the value of α may be identified when the number of observed sGRBs with known redshifts is more than 200. Finally, we compare our results of gamma-ray luminosity distribution with sGRBs with known redshifts, and found that our results are consistent with the observation, which implies that our simulation results can reproduce the observed luminosity distribution well.

Abstract Copyright: © 2020. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gamma-ray bursts - Gamma-ray astronomy - Astronomical methods

Simbad objects: 17

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Number of rows : 17
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 Fermi bn150120123 G 00 41 16.5630 +33 59 42.598           ~ 70 0
2 Fermi bn100117879 G 00 45 04.6610 -01 35 42.020           ~ 155 0
3 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 141 0
4 GRB 100625A gB 01 03 10.98 -39 05 18.3           ~ 124 0
5 PSO J047.1631+13.1580 G 03 08 39.14930640 +13 09 29.0253240           ~ 144 0
6 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
7 GALEX J123205.0-105600 Bz? 12 32 04.9717245480 -10 56 00.722548932         16.421 ~ 186 0
8 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
9 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
10 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
11 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
12 Fermi bn131004904 gB 19 44 27.20 -02 57 31.0           ~ 113 0
13 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
14 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
15 Fermi bn160624477 gB 22 00 46.21 +29 38 37.8           ~ 69 0
16 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
17 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1

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