2003ApJ...590..379B


Query : 2003ApJ...590..379B

2003ApJ...590..379B - Astrophys. J., 590, 379-385 (2003/June-2)

A standard kinetic energy reservoir in gamma-ray burst afterglows.

BERGER E., KULKARNI S.R. and FRAIL D.A.

Abstract (from CDS):

We present a comprehensive sample of X-ray observations of 41 γ-ray burst (GRB) afterglows, as well as jet opening angles, θj, for a subset with measured jet breaks. We show that there is a significant dispersion in the X-ray fluxes, and hence isotropic X-ray luminosities (LX,iso), normalized to t=10 hr. However, there is a strong correlation between LX,isoand the beaming fractions, fb≡[1-cos(θj)]. As a result, the true X-ray luminosity of GRB afterglows, LX=fbLX,iso, is approximately constant, with a dispersion of only a factor of 2. Since εeEb∝LX, the strong clustering of LXdirectly implies that the adiabatic blast wave kinetic energy in the afterglow phase, Eb, is tightly clustered. The narrow distribution of LXalso suggests that p~2, that inverse Compton emission does not in general dominate the observed X-ray luminosity, and that radiative losses at t<10 hr are relatively small. Thus, despite the large diversity in the observed properties of GRBs and their afterglows, the energy imparted by the GRB central engine to the relativistic ejecta is approximately constant.

Abstract Copyright: ∼

Journal keyword(s): Gamma Rays: Bursts - ISM: Jets and Outflows - Shock Waves

Simbad objects: 41

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Number of rows : 41
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 000529 gB 00 09 48.3 -61 27 53           ~ 17 0
2 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
3 GRB 990627 gB 01 48 25.4 -77 04 38           ~ 19 1
4 GRB 000210 gB 01 59 15 -40 40.0           ~ 175 0
5 GRB 010220 gB 02 36 59.0 +61 46 00           ~ 40 0
6 GRB 990217 gB 03 02 52.3 -53 05 37           ~ 29 0
7 GRB 990806 gB 03 10.5 -68 07           ~ 36 0
8 GRB 970228 gB 05 01 46.7 +11 46 53           ~ 650 1
9 GRB 991216 gB 05 09 31.2983 +11 17 07.262           ~ 430 0
10 GRB 990705 gB 05 09 54.5 -72 07 53           ~ 229 1
11 GRB 991014 gB 06 51 03.0 +11 36 05           ~ 41 0
12 GRB 970508 gB 06 53 49.2 +79 16 19           ~ 883 1
13 GRB 980329 gB 07 02 41 +38 50.7           ~ 276 1
14 GRB 990907 gB 07 33.7 -69 47           ~ 20 0
15 GRB 000115 gB 08 03 30.0 -17 13 30           ~ 29 0
16 GRB 980326 gB 08 36 34.3 -18 51 24           ~ 268 0
17 GRB 001025 gB 08 36.6 -13 04           ~ 48 1
18 GRB 980613 gB 10 17 57.8 +71 27 26           ~ 204 1
19 GRB 000528 gB 10 45 08.0 -33 59 26           ~ 29 0
20 GRB 011211 gB 11 15 16 -21 56.0           ~ 305 0
21 GRB 971214 gB 11 56 26.4 +65 12 01           ~ 445 1
22 GRB 990704 gB 12 19 27.3 -03 50 22           ~ 50 0
23 GRB 971227 gB 12 57 15.0 +59 24 02           ~ 50 0
24 GRB 990510 gB 13 38 07.64 -80 29 48.8           ~ 499 1
25 GRB 020405 gB 13 58 03.12 -31 22 22.2   21.9 21.5     ~ 259 1
26 GRB 970402 gB 14 50 06.0 -69 20 00           ~ 70 1
27 GRB 010222 G 14 52 12.5 +43 01 06           ~ 364 1
28 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
29 GRB 970111 gB 15 28 15.0 +19 36 18           ~ 140 0
30 4B 970815 gB 16 06 54.0 +81 30 34           ~ 56 0
31 GRB 000926 gB 17 04 15 +51 46.0           ~ 373 0
32 GRB 010214 gB 17 40 58.0 +48 34 37           ~ 41 0
33 GRB 020322 gB 18 00 48.5 +81 06 13           ~ 44 0
34 GRB 970828 gB 18 08 31.6 +59 18 51           ~ 353 1
35 GRB 001109 gB 18 30 07.8 +55 17 56           ~ 39 0
36 GRB 000214 gB 18 54 27.0 -66 27 30           ~ 92 0
37 GRB 020813A gB 19 46 41.874 -19 36 04.81           ~ 316 0
38 GRB 980515 gB 21 16 49.0 -67 11 48           ~ 22 0
39 GRB 980519 gB 23 22 21.5 +77 15 43           ~ 203 0
40 GRB 981226 gB 23 29 37.2 -23 55 54           ~ 108 1
41 GRB 980703 gB 23 59 06.7 +08 35 07           ~ 453 1

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