2024MNRAS.535.2482Y


Query : 2024MNRAS.535.2482Y

2024MNRAS.535.2482Y - Mon. Not. R. Astron. Soc., 535, 2482-2493 (2024/December-2)

The X-ray re-brightening of GRB afterglow revisited: a possible signature from activity of the central engine.

YANG Z., LU H.-J., YANG X., SHEN J. and YI S.-X.

Abstract (from CDS):

Long-duration gamma-ray bursts (GRBs) are thought to be from core collapse of massive stars, and a rapidly spinning magnetar or black hole may be formed as the central engine. The extended emission in the prompt emission, flares, and plateaus in X-ray afterglow, are proposed to be as the signature of central engine re-activity. However, the direct evidence from observations of identifying the central engines remains an open question. In this paper, we systemically search for long-duration GRBs that consist of bumps in X-ray afterglow detected by Swift/XRT and find that the peak time of the X-ray bumps exhibit bimodal distribution (defined as 'early' and 'late' bumps) with division line at $t=7190$ s. Although we cannot rule out that such a bimodality arises from selection effects. We proposed that the long-duration GRBs with an early (or late) bumps may be originated from the fall-back accretion onto a new-born magnetar (or black hole). By adopting Monte Carlo Markov Chain (MCMC) method to fit the early (or late) bumps of X-ray afterglow with the fall-back accretion of magnetar (or black hole), it is found that the initial surface magnetic field and period of magnetars for most early bumps are clustered around $5.88\times 10^{13}$ G and 1.04 ms, respectively. Meanwhile, the derived accretion mass of black hole for late bumps is in the range of $[4\times 10^{-4}, 1.8\times 10^{-2}]\,{\rm M}_{\odot }$, and the typical fall-back radius is distributed range of $[1.04, 4.23]\times 10^{11}$ cm, which is consistent with the typical radius of a Wolf-Rayet star. However, we also find that the fall-back accretion magnetar model is disfavoured by the late bumps, but the fall-back accretion of black hole model cannot be ruled out to interpret the early bumps of X-ray afterglow.

Abstract Copyright: © 2024 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): (transients:) gamma-ray bursts

Simbad objects: 30

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Number of rows : 30
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 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
2 GRB 100901A gB 01 49 03.56 +22 45 30.6           ~ 170 0
3 GRB 120215A gB 02 00 14 +08 47.4           ~ 31 0
4 GRB 120224A gB 02 43 46.17 -17 45 40.6           ~ 38 0
5 SN 2019oyw SN* 02 58 10.510 -08 57 27.20           ~ 218 0
6 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
7 GRB 121027A gB 04 14 23.450 -58 49 47.17           ~ 136 0
8 GRB 150911A gB 04 29 44.15 +05 44 07.6           ~ 29 0
9 GRB 220117A gB 06 06 17.40 -28 26 14.6           ~ 27 0
10 GRB 170822A gB 06 17 29 +55 00.0           ~ 22 0
11 GRB 131018A gB 06 33 53.40 -19 53 48.5           ~ 27 0
12 GRB 081028 gB 08 07 34.40 +02 18 16.8           ~ 125 0
13 Fermi bn120118709 gB 08 19 29.05 -07 11 05.1           ~ 87 0
14 GRB 051016B gB 08 48 27.810 +13 39 20.00 20.45         ~ 153 0
15 GRB 170202A gB 10 10 06 +05 01.0           ~ 90 0
16 GRB 230414B gB 12 04 22.72 +53 09 15.7           ~ 30 0
17 GRB 140515A gB 12 24 15.48 +15 06 17.7           ~ 90 0
18 GRB 150626B gB 12 30 32.03 +66 46 18.6           ~ 18 0
19 GRB 070208 gB 13 11 32.607 +61 57 54.37 20.79 20.79 19.86     ~ 119 0
20 GRB 060206 gB 13 31 43.420 +35 03 03.60   19.99 17.09     ~ 330 0
21 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
22 GRB 201128A gB 14 52 25.83 +26 41 05.4           ~ 8 0
23 GRB 200917A gB 15 42 53.87 -04 42 03.3           ~ 10 0
24 GRB 130807A gB 17 59 12.40 -27 36 56.7           ~ 24 0
25 Fermi bn120326056 gB 18 15 37.06 +69 15 35.4           ~ 188 0
26 GRB 071010A gB 19 12 14.42 -32 24 06.2           ~ 138 0
27 GRB 120213A gB 20 04 02.83 +65 24 40.6           ~ 37 0
28 GRB 181110A gB 20 09 16.32 -36 53 48.2           ~ 45 0
29 Fermi bn161129300 gB 21 04 54.66 +32 08 05.5           ~ 65 0
30 GRB 121209A gB 21 47 08.94 -08 14 05.8           ~ 50 0

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