2013ApJ...779...28G


Query : 2013ApJ...779...28G

2013ApJ...779...28G - Astrophys. J., 779, 28 (2013/December-2)

Delayed energy injection model for gamma-ray burst afterglows.

GENG J.J., WU X.F., HUANG Y.F. and YU Y.B.

Abstract (from CDS):

The shallow decay phase and flares in the afterglows of gamma-ray bursts (GRBs) are widely believed to be associated with the later activation of the central engine. Some models of energy injection involve a continuous energy flow since the GRB trigger time, such as the magnetic dipole radiation from a magnetar. However, in the scenario involving a black hole accretion system, the energy flow from the fall-back accretion may be delayed for a fall-back time ∼tfb. Thus, we propose a delayed energy injection model. The delayed energy would cause a notable rise to the Lorentz factor of the external shock, which will "generate" a bump in the multiple band afterglows. If the delayed time is very short, our model degenerates to the previous models. Our model can explain the significant re-brightening in the optical and infrared light curves of GRB 081029 and GRB 100621A. A considerable fall-back mass is needed to provide the later energy; this indicates that GRBs accompanied with fall-back material may be associated with a low energy supernova so that the fraction of the envelope can survive during eruption. The fall-back time can give meaningful information on the properties of GRB progenitor stars.

Abstract Copyright: ∼

Journal keyword(s): accretion, accretion disks - gamma-ray burst: individual (081029, 100621A) - methods: numerical

Simbad objects: 6

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Number of rows : 6
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 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
2 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
3 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 336 1
4 SN 2012bz SN* 09 07 38.38 +14 01 07.5           SNIb/c 193 1
5 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
6 GRB 081029 gB 23 07 06 -68 10.7           ~ 121 0

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