2009MNRAS.393..598S


Query : 2009MNRAS.393..598S

2009MNRAS.393..598S - Mon. Not. R. Astron. Soc., 393, 598-606 (2009/February-3)

The dust scattering model cannot explain the shallow X-ray decay in GRB afterglows.

SHEN R.-F., WILLINGALE R., KUMAR P., O'BRIEN P.T. and EVANS P.A.

Abstract (from CDS):

A dust scattering model was recently proposed to explain the shallow X-ray decay (plateau) observed prevalently in Gamma-Ray Burst (GRB) early afterglows. In this model, the plateau is the scattered prompt X-ray emission by the dust located close (about 10 to a few hundred pc) to the GRB site. In this paper, we carefully investigate the model and find that the scattered emission undergoes strong spectral softening with time, due to the model's essential ingredient that harder X-ray photons have smaller scattering angle thus arrive earlier, while softer photons suffer larger angle scattering and arrive later. The model predicts a significant change, that is Δβ ∼ 2-3, in the X-ray spectral index from the beginning of the plateau towards the end of the plateau, while the observed data show close to zero softening during the plateau and the plateau-to-normal transition phase. The scattering model predicts a big difference between the harder X-ray light curve and the softer X-ray light curve, i.e. the plateau in harder X-rays ends much earlier than in softer X-rays. This feature is not seen in the data. The large scattering optical depths of the dust required by the model imply strong extinction in optical, AV≳ 10, which contradicts current findings of AV= 0.1-0.7 from optical and X-ray afterglow observations. We conclude that the dust scattering model cannot explain the X-ray plateaus.

Abstract Copyright: © 2009 The Authors. Journal compilation © 2009 RAS

Journal keyword(s): radiation mechanisms: non-thermal - scattering - dust, extinction - gamma-rays: burst

Simbad objects: 28

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Number of rows : 28
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 070129 gB 02 28 00.940 +11 41 04.00       21.3   ~ 120 0
2 GRB 060306 gB 02 44 22.830 -02 08 55.00           ~ 119 0
3 GRB 050822 gB 03 24 27.240 -46 01 59.20     20.82     ~ 115 0
4 GRB 060210 gB 03 50 57.370 +27 01 34.40   20.27       ~ 275 0
5 GRB 070328 gB 04 20 27.680 -34 04 00.60 20.29         ~ 97 0
6 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
7 GRB 060510A gB 06 23 27.980 -01 09 46.20 18.19   18.45     ~ 58 0
8 GRB 061202 gB 07 02 06.190 -74 41 54.91           ~ 83 0
9 GRB 060813 gB 07 27 35.380 -29 50 49.40           ~ 62 0
10 GRB 070420 gB 08 04 55.170 -45 33 19.99 20.39 20.01 17.16     ~ 83 0
11 GRB 060428A gB 08 14 10.840 -37 10 11.70     19.97     ~ 54 0
12 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
13 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
14 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
15 GRB 050802 gB 14 37 05.820 +27 47 12.62 16.85 17.38 16.97     ~ 186 0
16 GRB 050128 gB 14 38 17.750 -34 45 55.61           ~ 68 0
17 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 241 0
18 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
19 GRB 060502A gB 16 03 42.480 +66 36 02.49     18.65     ~ 143 0
20 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
21 GRB 060413 gB 19 25 07.850 +13 45 29.90           ~ 69 0
22 GRB 050315 gB 20 25 54.100 -42 36 02.19           ~ 225 0
23 GRB 050713B gB 20 31 15.570 +60 56 43.70           ~ 72 0
24 GRB 070508 gB 20 51 11.810 -78 23 04.88     19.62     ~ 144 0
25 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
26 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
27 GRB 050803 gB 23 22 37.910 +05 47 09.00           ~ 127 0
28 GRB 061222A gB 23 53 03.419 +46 31 58.60           ~ 177 0

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