2010ApJ...712.1172D


Query : 2010ApJ...712.1172D

2010ApJ...712.1172D - Astrophys. J., 712, 1172-1190 (2010/April-1)

Flares in long and short gamma-ray bursts.

DADO S. and DAR A.

Abstract (from CDS):

The many similarities between the prompt emission pulses in gamma-ray bursts (GRBs) and X-ray flares during the fast decay and afterglow (AG) phases of GRBs suggest a common origin. In the cannonball (CB) model of GRBs, this common origin is mass accretion episodes of fall-back matter on a newly born compact object. The prompt emission pulses are produced by a bipolar jet of highly relativistic plasmoids (CBs) ejected in the early, major episodes of mass accretion. As the accretion material is consumed, one may expect the engine's activity to weaken. X-ray flares ending the prompt emission and during the AG phase are produced in such delayed episodes of mass accretion. The common engine, environment, and radiation mechanisms (inverse Compton scattering and synchrotron radiation) produce their observed similarities. Flares in both long GRBs and short hard gamma-ray bursts (SHBs) can also be produced by bipolar ejections of CBs following a phase transition in compact objects due to loss of angular momentum and/or cooling. Optical flares, however, are mostly produced in collisions of CBs with massive stellar winds/ejecta or with density bumps along their path. In this paper, we show that the master formulae of the CB model of GRBs and SHBs, which reproduce very well their prompt emission pulses and their smooth AGs, seem to reproduce also very well the light curves and spectral evolution of the prominent X-ray and optical flares that are well sampled.

Abstract Copyright:

Journal keyword(s): gamma-ray burst: general

Simbad objects: 37

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Number of rows : 37
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 GRB 071031 gB 00 25 37.40 -58 03 33.9           ~ 166 0
2 Fermi bn090621185 gB 00 43 56.80 +61 56 17.6           ~ 57 0
3 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 289 1
4 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 147 0
5 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 282 0
6 GRB 970508 gB 06 53 49.2 +79 16 19           ~ 868 1
7 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 221 0
8 GRB 050916 gB 09 03 57.270 -51 25 42.51           ~ 45 0
9 GRB 050502B gB 09 30 10.024 +16 59 48.07           ~ 161 0
10 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1208 1
11 GRB 030418 gB 10 54 33.69 -07 01 40.8           ~ 68 0
12 GRB 080330 gB 11 17 06.70 +30 36 24.1           ~ 133 0
13 GRB 011121 gB 11 34 26.67 -76 01 41.6       23.0   ~ 275 1
14 GRB 080607A gB 12 59 47.14 +15 55 09.6           ~ 235 0
15 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 313 0
16 GRB 080319A gB 13 45 19.97 +44 04 49.1           ~ 76 0
17 GRB 090417B gB 13 58 44.8 +47 00 55           ~ 112 1
18 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 467 0
19 GRB 080906 gB 15 12 13 -80 32.4           ~ 52 0
20 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 989 1
21 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 269 0
22 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 157 0
23 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 360 0
24 GRB 000301C gB 16 20 18.5 +29 26 35           ~ 356 0
25 GRB 050724 gB 16 24 44.400 -27 32 27.90     19.70     ~ 439 1
26 GRB 060929 gB 17 32 28.920 +29 50 06.20           ~ 58 0
27 GRB 090709A gB 19 19 46.70 +60 43 40.8           ~ 114 0
28 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1821 2
29 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 320 0
30 GRB 071003 gB 20 07 24.50 +10 56 48.8           ~ 170 0
31 GRB 060614 gB 21 23 32.140 -53 01 36.10 18.89 20.12 19.54     ~ 612 1
32 GRB 080506 gB 21 57 41.79 +38 59 06.7           ~ 44 0
33 Fermi bn081102739 gB 22 04 42.60 +52 59 27.7           ~ 55 0
34 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 386 0
35 GRB 090812 gB 23 32 48.5 -10 36 17           ~ 143 0
36 GRB 070704 gB 23 38 47.31 +66 15 12.7           ~ 56 0
37 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 213 0

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