2018MNRAS.481.4332A


Query : 2018MNRAS.481.4332A

2018MNRAS.481.4332A - Mon. Not. R. Astron. Soc., 481, 4332-4341 (2018/December-3)

Merger delay time distribution of extended emission short GRBs.

ANAND N., SHAHID M. and RESMI L.

Abstract (from CDS):

The most popular progenitor model for short-duration gamma-ray bursts (sGRBs) is the merger of two compact objects. The spatial and temporal coincidence of GRB 170817A with the binary neutron star merger GW170817 has strengthened this model. However, the short GRB population exhibits a certain diversity: some bursts display an extended emission (EE), continuing in soft gamma-rays for a few hundreds of seconds post the short initial pulse. It is currently unclear whether the origin of such bursts is in compact object mergers. Within the merger model, the redshift (z) distribution of short GRBs is influenced by the merger delay time, i.e. time elapsed between the merger and the formation of the binary star system, which is dominated by the time-scale for gravitational wave losses during the compact binary phase. We examine redshift distributions of short GRBs with EE to see whether their formation channel requires considerable delay post the star formation episode. Our results show that the z-distribution of EE bursts is consistent with the merger model. We attempted to compare the delay time distribution of the EE and the non-EE short bursts. However, no statistically significant difference could be seen within the limited sample size. For general short GRB z-distribution, we find that luminosity functions extending to lower values prefer shorter delay times compared to those terminated at higher luminosities.

Abstract Copyright: © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): gravitational waves - gamma rays: bursts

Simbad objects: 45

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Number of rows : 45
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 J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
6 GRB 141212A G 02 36 29.9570 +18 08 47.228           ~ 70 0
7 PSO J047.1631+13.1580 G 03 08 39.14930640 +13 09 29.0253240           ~ 144 0
8 GRB 070729 gB 03 45 16.04 -39 19 19.9           ~ 81 0
9 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
10 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
11 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
12 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
13 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
14 GRB 160410A gB 10 02 44.37 +03 28 42.7           ~ 75 0
15 GRB 061217 gB 10 41 39.320 -21 07 22.11           ~ 128 0
16 GRB 090515 gB 10 56 41.0 +14 27 22           ~ 122 0
17 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
18 GRB 090530 gB 11 57 36.00 +26 35 23.0           ~ 89 0
19 GALEX J123205.0-105600 Bz? 12 32 04.9717245480 -10 56 00.722548932         16.421 ~ 186 0
20 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
21 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
22 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
23 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
24 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
25 GRB 150423A gB 14 46 18.96 +12 17 00.6           ~ 79 0
26 GRB 120804A G 15 35 47.5100 -28 46 56.110           ~ 99 0
27 GRB 140903A G 15 52 03.2650 +27 36 10.710           ~ 138 0
28 GRB 050813 gB 16 07 57.190 +11 14 57.80           ~ 147 0
29 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
30 GRB 060502B gB 18 35 46.060 +52 37 51.45           ~ 153 1
31 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
32 Fermi bn131004904 gB 19 44 27.20 -02 57 31.0           ~ 113 0
33 GRB 140622A gB 21 08 41.56 -14 25 09.5           ~ 61 0
34 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
35 GRB 070429B G 21 52 03.6910 -38 49 42.820           ~ 125 0
36 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
37 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 138 0
38 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 286 1
39 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
40 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
41 GRB 080123 gB 22 35 46.100 -64 54 03.24           ~ 98 0
42 Fermi bn090927422 gB 22 55 53.41 -70 58 49.3           ~ 112 0
43 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1
44 GRB 070506 gB 23 08 52.390 +10 43 20.30     19.04     ~ 86 0
45 Fermi bn100816026 gB 23 26 57.56 +26 34 42.6           ~ 170 0

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