2007MNRAS.377.1464N


Query : 2007MNRAS.377.1464N

2007MNRAS.377.1464N - Mon. Not. R. Astron. Soc., 377, 1464-1472 (2007/June-1)

The role of afterglow break-times as gamma-ray burst jet angle indicators.

NAVA L., GHISELLINI G., GHIRLANDA G., CABRERA J.I., FIRMANI C. and AVILA-REESE V.

Abstract (from CDS):

The early X-ray light curve of gamma-ray bursts (GRBs) is complex, and shows a typical steep-flat-steep behaviour. The time Ta at which the flat (plateau) part ends may bear some important physical information, especially if it plays the same role of the so called jet break-time tjet. To this aim, stimulated by the recent analysis of Willingale et al., we have assembled a sample of GRBs of known redshifts, spectral parameters of the prompt emission, and Ta. By using Ta as a jet angle indicator, and then estimating the collimation-corrected prompt energetics, we find a correlation between the latter quantity and the peak energy of the prompt emission. However, this correlation has a large dispersion, similar to the dispersion of the Amati correlation and it is not parallel to the Ghirlanda correlation. Furthermore, we show that the correlation itself results mainly from the dependence of the jet opening angle on the isotropic prompt energy, with the time Ta playing no role, contrary to what we find for the jet break-time tjet. We also find that for the bursts in our sample Ta weakly correlates with Eγ,isoof the prompt emission, but that this correlation disappears when considering all bursts of known redshift and Ta. There is no correlation between Ta and the isotropic energy of the plateau phase.

Abstract Copyright: 2007 The Authors. Journal compilation © 2007 RAS

Journal keyword(s): radiation mechanisms: general - gamma-rays: bursts - X-rays: general

Simbad objects: 23

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Number of rows : 23
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 050908 gB 01 21 50.750 -12 57 17.20           ~ 179 0
2 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
3 GRB 050603 gB 02 39 56.839 -25 10 54.92     18.48     ~ 174 0
4 GRB 050318 gB 03 18 51.000 -46 23 43.61 18.10 18.68 17.58     ~ 189 0
5 GRB 060115 gB 03 36 08.400 +17 20 43.00           ~ 179 0
6 GRB 060223A gB 03 40 49.560 -17 07 48.40     17.90     ~ 98 0
7 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
8 GRB 050505 gB 09 27 03.300 +30 16 23.70     20.74     ~ 206 0
9 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
10 GRB 050416 gB 12 33 54.600 +21 03 26.69     19.12     ~ 300 1
11 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
12 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
13 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
14 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
15 GRB 050126 gB 18 32 27.22 +42 22 14.2           ~ 129 0
16 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
17 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
18 GRB 060522 gB 21 31 44.850 +02 53 10.80           ~ 140 0
19 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 215 0
20 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
21 GRB 051109A gB 22 01 15.320 +40 49 23.70   20.09 20.14     ~ 190 0
22 GRB 050820A gB 22 29 38.110 +19 33 37.10 18.33 19.00 18.47     ~ 409 0
23 GRB 060707 gB 23 48 19.000 -17 54 17.00     19.79     ~ 170 0

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