2020MNRAS.493..783M


Query : 2020MNRAS.493..783M

2020MNRAS.493..783M - Mon. Not. R. Astron. Soc., 493, 783-791 (2020/March-3)

Linking extended and plateau emissions of short gamma-ray bursts.

MATSUMOTO T., KIMURA S.S., MURASE K. and MESZAROS P.

Abstract (from CDS):

Some short gamma-ray bursts (SGRBs) show a longer lasting emission phase, called extended emission (EE) lasting ∼102–3 s, as well as a plateau emission (PE) lasting ∼ 104–5 s. Although a long-lasting activity of the central engines is a promising explanation for powering both emissions, their physical origin and their emission mechanisms are still uncertain. In this work, we study the properties of the EEs and their connection with the PEs. First, we constrain the minimal Lorentz factor Γ of the outflows powering EEs, using compactness arguments and find that the outflows should be relativistic, Γ >= 10. We propose a consistent scenario for the PEs, where the outflow eventually catches up with the jet responsible for the prompt emission, injecting energy into the forward shock formed by the prior jet, which naturally results in a PE. We also derive the radiation efficiency of EEs and the Lorentz factor of the outflow within our scenario for 10 well-observed SGRBs accompanied by both EE and PE. The efficiency has an average value of ∼3 per cent but shows a broad distribution ranging from ∼0.01 to ∼100 per cent. The Lorentz factor is ∼20-30, consistent with the compactness arguments. These results suggest that EEs are produced by a slower outflow via more inefficient emission than the faster outflow that causes the prompt emission with a high radiation efficiency.

Abstract Copyright: © 2020 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): gravitational waves - relativistic processes - gamma-ray bursts

Simbad objects: 44

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Number of rows : 44
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 bn100522157 gB 00 27 56.79 +09 24 06.6           ~ 57 0
2 GRB 110207A gB 00 50 09.50 -10 47 23.8           ~ 37 0
3 GRB 970918 gB 02 06.0 +40 11           ~ 3 0
4 GRB 961017 gB 02 26 -12.9           ~ 11 0
5 1B 911119 gB 02 49.7 +67 46           ~ 17 0
6 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
7 GRB 060313 G 04 26 28.4020 -10 50 39.901 20.55 21.03 19.66     ~ 156 0
8 GRB 960906 gB 04 33 -39.3           ~ 9 0
9 4B 951211 gB 05 24.6 -18 56           ~ 11 0
10 GRB 090820 gB 05 51 +27.1           ~ 44 0
11 Fermi bn080807993 gB 06 47 -16.0           ~ 25 0
12 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
13 GRB 980904 gB 08 34 -62.8           ~ 11 0
14 GRB 051016B gB 08 48 27.810 +13 39 20.00 20.45         ~ 153 0
15 1B 910725 gB 09 01.4 -19 29           ~ 18 0
16 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
17 GRB 090831A gB 09 40 23 +50 58.0           ~ 36 0
18 GRB 110824A gB 10 08 +01.3           ~ 15 0
19 UCAC4 217-047923 * 10 19 02.5992684123 -46 40 11.294771086   13.795 12.458 12.114   ~ 54 0
20 GRB 121014A gB 11 06 34.70 -29 06 18.3           ~ 20 0
21 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
22 GRB 110402A gB 13 09 36.54 +61 15 10.3           ~ 67 0
23 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
24 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
25 Fermi bn121029350 gB 15 07 -28.2           ~ 13 0
26 GRB 091120 gB 15 07.2 -21 47           ~ 34 0
27 GRB 140903A G 15 52 03.2650 +27 36 10.710           ~ 138 0
28 Fermi bn120605453 gB 16 14 +41.5           ~ 13 0
29 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
30 GRB 090531B gB 16 48 15.0 -36 01 27           ~ 58 0
31 GRB 980112 gB 17 47 53 +10 42.6           ~ 5 0
32 4B 950531 gB 18 18.8 +17 47           ~ 10 0
33 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
34 GRB 080503 gB 19 06 28.74 +68 47 35.8           ~ 172 0
35 1B 911016 gB 20 01.9 -03 47           ~ 47 0
36 GRB 120402A gB 20 57 18.0 +19 15 28           ~ 7 0
37 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
38 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
39 Fermi bn090927422 gB 22 55 53.41 -70 58 49.3           ~ 112 0
40 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1
41 GRB 070506 gB 23 08 52.390 +10 43 20.30     19.04     ~ 86 0
42 GRB 090131 gB 23 29.2 +21 12           ~ 37 0
43 Fermi bn100212588 gB 23 45 40.39 +49 29 39.6           ~ 56 0
44 GRB 100517A gB ~ ~           ~ 5 0

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