2024MNRAS.527.1638Z


Query : 2024MNRAS.527.1638Z

2024MNRAS.527.1638Z - Mon. Not. R. Astron. Soc., 527, 1638-1647 (2024/January-2)

A two-component jet model for the optical plateau in the afterglow of GRB 191221B.

ZHU Y.-M., WANG Y., ZHOU H., LIPUNOV V., BUCKLEY D.A.H., BALANUTSA P., JIN Z.-P. and WEI D.-M.

Abstract (from CDS):

The long gamma-ray burst GRB 191221B has abundant observations in X-ray, optical, and radio bands. In the literature, the observed optical light curve of GRB 191221B displays a plateau around 0.1 d, which is rather peculiar in gamma-ray bursts. Here, we performed detailed analysis of the observational data from Swift/UVOT, Very Large Telescope, and Las Cumbres Observatory, obtained the light curve of the multiband afterglow of GRB 191221B. By examining optical, ultraviolet, X-ray, and radio data for this event, we demonstrate that an on-axis two-component jet model can explain the observations. Our analysis suggests that the narrow component has an initial Lorentz factor of 400 and a jet opening half-angle of 1.4°, while the wide component has an initial Lorentz factor of 25 and a jet opening half-angle of 2.8°. The narrow jet dominates the early decay, whereas the wider jet causes the optical plateau and dominates late decay. According to this model, the reason for the absence of the X-ray plateau is due to the steeper spectral index of the wide component, resulting in a less significant flux contribution from the wide jet in the X-ray bands than in the optical bands. Moreover, we have explained the inconsistency in the decay indices of the UVOT- and Rc-band data around 2000 s using reverse shock emission.

Abstract Copyright: © The Author(s) 2023. Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): gamma-ray burst: individual: GRB 191221B - ISM: jets and outflows

Simbad objects: 2

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Number of rows : 2
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 191221B gB 10 19 19.17 -38 09 27.5           ~ 66 0
2 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1

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