2013ApJ...776..120Y


Query : 2013ApJ...776..120Y

2013ApJ...776..120Y - Astrophys. J., 776, 120 (2013/October-3)

Early afterglows of gamma-ray bursts in a stratified medium with a power-law density distribution.

YI S.-X., WU X.-F. and DAI Z.-G.

Abstract (from CDS):

A long-duration gamma-ray burst (GRB) has been widely thought to arise from the collapse of a massive star, and it has been suggested that its ambient medium is a homogenous interstellar medium (ISM) or a stellar wind. There are two shocks when an ultra-relativistic fireball that has been ejected during the prompt gamma-ray emission phase sweeps up the circumburst medium: a reverse shock that propagates into the fireball, and a forward shock that propagates into the ambient medium. In this paper, we investigate the temporal evolution of the dynamics and emission of these two shocks in an environment with a general density distribution of n∝R –k (where R is the radius) by considering thick-shell and thin-shell cases. A GRB afterglow with one smooth onset peak at early times is understood to result from such external shocks. Thus, we can determine the medium density distribution by fitting the onset peak appearing in the light curve of an early optical afterglow. We apply our model to 19 GRBs and find that their k values are in the range of 0.4-1.4, with a typical value of k ∼ 1, implying that this environment is neither a homogenous ISM with k = 0 nor a typical stellar wind with k = 2. This shows that the progenitors of these GRBs might have undergone a new mass-loss evolution.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: general - radiation mechanisms: non-thermal

Simbad objects: 19

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Number of rows : 19
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 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
2 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 136 0
3 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
4 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
5 GRB 070318 gB 03 13 56.830 -42 56 46.30 18.27 16.23 15.49     ~ 170 0
6 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
7 GRB 070411 gB 07 09 19.930 +01 03 52.60     17.94     ~ 138 0
8 GRB 070420 gB 08 04 55.170 -45 33 19.99 20.39 20.01 17.16     ~ 83 0
9 GRB 030418 gB 10 54 33.69 -07 01 40.8           ~ 69 0
10 GRB 080330 gB 11 17 06.70 +30 36 24.1           ~ 145 0
11 GRB 070419A gB 12 10 58.830 +39 55 34.06 18.52         ~ 130 0
12 GRB 090313 gB 13 13 36.00 +08 05 10.7           ~ 149 0
13 GRB 080319A gB 13 45 19.97 +44 04 49.1           ~ 79 0
14 GRB 050730 gB 14 08 17.090 -03 46 18.90   20.32 17.68     ~ 327 0
15 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 177 0
16 GRB 071010A gB 19 12 14.42 -32 24 06.2           ~ 138 0
17 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
18 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 210 0
19 Fermi bn080810549 gB 23 47 08.00 +00 18 35.1           ~ 240 0

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