2009MNRAS.392..153D


Query : 2009MNRAS.392..153D

2009MNRAS.392..153D - Mon. Not. R. Astron. Soc., 392, 153-169 (2009/January-1)

Jet breaks at the end of the slow decline phase of Swift GRB light curves.

DE PASQUALE M., EVANS P., OATES S., PAGE M., ZANE S., SCHADY P., BREEVELD A., HOLLAND S., KUIN P., STILL M., ROMING P. and WARD P.

Abstract (from CDS):

The Swift mission has discovered an intriguing feature of gamma-ray burst (GRBs) afterglows, a phase of shallow decline of the flux in the X-ray and optical light curves. This behaviour is typically attributed to energy injection into the burst ejecta. At some point this phase ends, resulting in a break in the light curve, which is commonly interpreted as the cessation of the energy injection. In a few cases, however, while breaks in the X-ray light curve are observed, optical emission continues its slow flux decline. This behaviour suggests a more complex scenario. In this paper, we present a model that invokes a double component outflow, in which narrowly collimated ejecta are responsible for the X-ray emission while a broad outflow is responsible for the optical emission. The narrow component can produce a jet break in the X-ray light curve at relatively early times, while the optical emission does not break due to its lower degree of collimation. In our model both components are subject to energy injection for the whole duration of the follow-up observations. We apply this model to GRBs with chromatic breaks, and we show how it might change the interpretation of the GRBs canonical light curve. We also study our model from a theoretical point of view, investigating the possible configurations of frequencies and the values of GRB physical parameters allowed in our model.

Abstract Copyright: © 2008 The Authors. Journal compilation © 2008 RAS

Journal keyword(s): gamma-rays: bursts

Simbad objects: 10

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Number of rows : 10
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 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
2 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
3 GRB 050802 gB 14 37 05.820 +27 47 12.62 16.85 17.38 16.97     ~ 186 0
4 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 348 0
5 GRB 050607 gB 20 00 42.790 +09 08 31.50   19.55 18.94     ~ 103 0
6 GRB 050922C gB 21 09 33.000 -08 45 30.10 15.15 15.86 14.69     ~ 301 0
7 GRB 050713A gB 21 22 09.530 +77 04 29.50           ~ 125 0
8 GRB 050713 gB 21 22 09.78 +77 04 28.9           ~ 11 0
9 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 210 0
10 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 286 1

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