2024ApJ...962....6Y


Query : 2024ApJ...962....6Y

2024ApJ...962....6Y - Astrophys. J., 962, 6 (2024/February-2)

Can Fallback Accretion on the Magnetar Model Power the X-Ray Flares Simultaneously Observed with Gamma Rays of Gamma-Ray Bursts?

YU W.-Y., LU H.-J., YANG X., LAN L. and YANG Z.

Abstract (from CDS):

The prompt emission, X-ray plateau, and X-ray flares of gamma-ray bursts (GRBs) are thought to be from internal dissipation, and the magnetar as the central engine with propeller fallback accretion is proposed to interpret the observed phenomena of GRBs. In this paper, by systematically searching for X-ray emission observed by Swift/X-ray Telescope, we find that seven robust GRBs include both X-ray flares and plateau emissions with measured redshift. More interestingly, the X-ray flares/bumps for those seven GRBs are simultaneously observed in the gamma-ray band. By adopting the propeller fallback accretion model to fit the observed data, it is found that the free parameters of two GRBs (140512A and 180329B) can be constrained very well, while in the other five cases, more or less, they are not all sufficiently constrained. On the other hand, this requires the conversion efficiency of the propeller to be two or three times higher than that of the spindown dipole radiation of the magnetar. If this is the case, it is contradictory to the expectation from the propeller model: namely, a dirtier ejecta should be less efficient in producing gamma-ray emissions. Our results hint that at least the magnetar central engine with propeller fallback accretion model cannot interpret very well both the GRB X-ray flares simultaneously observed in the gamma-ray band and the X-ray flares of GRBs with a high Lorentz factor.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gamma-ray bursts

Simbad objects: 11

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Number of rows : 11
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 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
2 Fermi bn130609902 gB 03 35 05.11 -40 10 26.7           ~ 54 0
3 GRB 180329B gB 05 31 36.91 -23 41 27.4           ~ 49 0
4 GRB 061202 gB 07 02 06.190 -74 41 54.91           ~ 83 0
5 GRB 211227A gB 08 48 35.73 -02 44 07.1           ~ 57 0
6 GRB 180325A gB 10 29 42.57 +24 27 48.7           ~ 85 0
7 SDSS J140910.47+275320.8 G 14 09 10.47535 +27 53 20.8393           ~ 279 0
8 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
9 Fermi bn140512814 gB 19 17 28.81 -15 05 39.5           ~ 133 0
10 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
11 GRB 191019A gB 22 40 05.87 -17 19 40.8           ~ 55 0

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