2002ApJ...570..573G


Query : 2002ApJ...570..573G

2002ApJ...570..573G - Astrophys. J., 570, 573-587 (2002/May-2)

Extended power-law decays in BATSE gamma-ray bursts: signatures of external shocks.

GIBLIN T.W., CONNAUGHTON V., VAN PARADIJS J., PREECE R.D., BRIGGS M.S., KOUVELIOTOU C., WIJERS R.A.M.J. and FISHMAN G.J.

Abstract (from CDS):

The connection between gamma-ray bursts (GRBs) and their afterglows is currently not well understood. Afterglow models of synchrotron emission generated by external shocks in the GRB fireball model predict emission detectable in the gamma-ray regime (≳25 keV). In this paper, we present a temporal and spectral analysis of a subset of BATSE GRBs with smooth extended emission tails to search for signatures of the ``early high-energy afterglow'', i.e., afterglow emission that initially begins in the gamma-ray phase and subsequently evolves into X-ray, UV, optical, and radio emission as the blast wave is decelerated by the ambient medium. From a sample of 40 GRBs we find that the temporal decays are best described with a power law ~tβ rather than an exponential with a mean index <β>~-2. Spectral analysis shows that ∼20% of these events are consistent with fast-cooling synchrotron emission for an adiabatic blast wave, three of which are consistent with the blast-wave evolution of a jet with Fν∼t–p. This behavior suggests that in some cases, the emission may originate from a narrow jet, possibly consisting of ``nuggets'' whose angular sizes are less than 1/Γ, where Γ is the bulk Lorentz factor.

Abstract Copyright: ∼

Journal keyword(s): Gamma Rays: Bursts

Simbad objects: 47

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Number of rows : 47
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 980306 gB 00 34 -46.2           ~ 21 0
2 GRB 990322 gB 01 15 -70.3           ~ 7 0
3 1B 920218 gB 02 37.9 +27 28           ~ 23 0
4 4B 951104 gB 02 41.6 +27 16           ~ 14 0
5 1B 910927 gB 03 20.6 -39 39           ~ 41 0
6 1B 910814C gB 03 52.0 +45 13           ~ 30 0
7 GRB 970411 gB 03 56 +34.3           ~ 15 0
8 GRB 990415 gB 04 58 -02.1           ~ 9 0
9 GRB 970228 gB 05 01 46.7 +11 46 53           ~ 650 1
10 GRB 980923 gB 05 07.8 -80 36           ~ 51 0
11 GRB 991216 gB 05 09 31.2983 +11 17 07.262           ~ 430 0
12 GRB 981205 gB 06 33 +45.3           ~ 10 0
13 GRB 980301 gB 06 45 -30.9           ~ 17 0
14 3B 930612 gB 06 52.3 -69 46           ~ 48 0
15 3B 940419B gB 07 01.4 +51 26           ~ 8 0
16 GRB 980329 gB 07 02 41 +38 50.7           ~ 276 1
17 GRB 930106B gB 08 19.2 -32 37           ~ 16 0
18 V* GP Vel HXB 09 02 06.8608812864 -40 33 16.899168060 6.85 7.37 6.87 6.31 6.05 B0.5Ia 1588 0
19 1B 910602 gB 09 31.0 +53 59           ~ 25 0
20 4B 960530 gB 09 33.6 -53 47           ~ 31 0
21 GRB 990316 gB 10 11 -05.5           ~ 27 0
22 2B 920502 gB 10 19.3 +45 25           ~ 20 0
23 2B 920801 gB 10 31.4 +68 54           ~ 24 0
24 2B 920622 gB 10 48.4 +47 10           ~ 54 0
25 GRB 981203 gB 11 00 +32.0           ~ 14 0
26 GRB 000103 gB 11 01 -58.2           ~ 11 0
27 GRB 990220 gB 11 04 +57.6           ~ 13 0
28 2B 930131 gB 12 08.2 -08 14           ~ 127 0
29 4B 941026 gB 13 43.8 -06 32           ~ 37 0
30 2B 920813 gB 13 44.9 -28 20           ~ 12 0
31 GRB 980325 gB 14 05 -51.4           ~ 11 0
32 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
33 GRB 971127 gB 15 32 +32.2           ~ 24 0
34 3B 931223 gB 17 07.2 +41 14           ~ 10 0
35 2B 920901 gB 17 26.6 +16 04           ~ 14 0
36 GRB 990102 gB 18 22 +39.7           ~ 25 0
37 GRB 970302 gB 18 55 +34.9           ~ 8 0
38 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
39 1B 911016 gB 20 01.9 -03 47           ~ 47 0
40 2B 921207 gB 20 25.3 -42 56           ~ 47 0
41 GRB 970925 gB 22 02 -11.7           ~ 24 0
42 GRB 991229 gB 22 12.0 +33 38           ~ 8 0
43 GRB 980306B gB 22 48 -58.6           ~ 20 0
44 GRB 990518 gB 23 16 -37.1           ~ 13 0
45 3B 940218 gB 23 18.8 -19 41           ~ 9 0
46 GRB 980519 gB 23 22 21.5 +77 15 43           ~ 203 0
47 GRB 971208 gB 23 45 50 +77 56.4           ~ 18 0

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