2018MNRAS.475..266Z


Query : 2018MNRAS.475..266Z

2018MNRAS.475..266Z - Mon. Not. R. Astron. Soc., 475, 266-276 (2018/March-3)

Search for the signatures of a new-born black hole from the collapse of a supra-massive millisecond magnetar in short GRB light curves.

ZHANG Q., LEI W.H., ZHANG B.B., CHEN W., XIONG S.L. and SONG L.M.

Abstract (from CDS):

'Internal plateau' followed by a sharp decay is commonly seen in short gamma-ray burst (GRB) light curves. The plateau component is usually interpreted as the dipole emission from a supra-massive magnetar, and the sharp decay may imply the collapse of the magnetar to a black hole (BH). Fall-back accretion on to the new-born BH could produce long-lasting activities via the Blandford-Znajek (BZ) process. The magnetic flux accumulated near the BH would be confined by the accretion discs for a period of time. As the accretion rate decreases, the magnetic flux is strong enough to obstruct gas infall, leading to a magnetically arrested disc. Within this scenario, we show that the BZ process could produce two types of typical X-ray light curves: type I exhibits a long-lasting plateau, followed by a power-law (PL) decay with slopes ranging from 5/3 to 40/9; type II shows roughly a single PL decay with a slope of 5/3. The former requires low magnetic field strength, while the latter corresponds to relatively high values. We search for such signatures of the new-born BH from a sample of short GRBs with an internal plateau, and find two candidates: GRB 101219A and GRB 160821B, corresponding to type II and type I light curves, respectively. It is shown that our model can explain the data very well.

Abstract Copyright: © 2017 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): accretion, accretion discs - gamma-ray burst: individual: ((GRB 101219A, GRB 160821B)) - stars: magnetars

Simbad objects: 14

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Number of rows : 14
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 070110 gB 00 03 39.270 -52 58 27.00 21.8 21.9 21.2     ~ 220 0
2 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
3 Fermi bn081024245 gB 01 51 33.80 +61 21 08.2           ~ 75 0
4 GRB 120305A gB 03 10 08.73 +28 29 30.9           ~ 56 0
5 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
6 GRB 120521A gB 09 54 53.91 -49 25 02.4           ~ 41 0
7 GRB 090515 gB 10 56 41.0 +14 27 22           ~ 122 0
8 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
9 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
10 GRB 100702A gB 16 22 47.26 -56 31 53.8           ~ 53 0
11 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
12 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
13 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
14 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 138 0

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