2018MNRAS.478.4323G


Query : 2018MNRAS.478.4323G

2018MNRAS.478.4323G - Mon. Not. R. Astron. Soc., 478, 4323-4335 (2018/August-3)

Fallback accretion on to a newborn magnetar: long GRBs with giant X-ray flares.

GIBSON S.L., WYNN G.A., GOMPERTZ B.P. and O'BRIEN P.T.

Abstract (from CDS):

Flares in the X-ray afterglow of gamma-ray bursts (GRBs) share more characteristics with the prompt emission than the afterglow, such as pulse profile and contained fluence. As a result, they are believed to originate from late-time activity of the central engine and can be used to constrain the overall energy budget. In this paper, we collect a sample of 19 long GRBs observed by Swift-XRT that contain giant flares in their X-ray afterglows. We fit this sample with a version of the magnetar propeller model, modified to include fallback accretion. This model has already successfully reproduced extended emission in short GRBs. Our best-fittings provide a reasonable morphological match to the light curves. However, 16 out of 19 of the fits require efficiencies for the propeller mechanism that approach 100 percent. The high-efficiency parameters are a direct result of the high energy contained in the flares and the extreme duration of the dipole component, which forces either slow spin periods or low-magnetic fields. We find that even with the inclusion of significant fallback accretion, in all but a few cases it is energetically challenging to produce prompt emission, afterglow, and giant flares within the constraints of the rotational energy budget of a magnetar.

Abstract Copyright: © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): accretion, accretion discs - gamma-ray burst: general - stars: magnetars

Simbad objects: 19

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Number of rows : 19
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 Fermi bn090621185 gB 00 43 56.80 +61 56 17.6           ~ 59 0
2 GRB 060904B gB 03 52 50.520 -00 43 30.61 18.27 19.14 18.37     ~ 208 0
3 GRB 060124 gB 05 08 25.900 +69 44 26.98   18.91 17.35     ~ 280 0
4 Fermi bn100619015 gB 05 38 28.0 -27 00 02           ~ 57 0
5 GRB 110801A gB 05 57 44.87 +80 57 21.1           ~ 90 0
6 GRB 070520B gB 08 07 31.070 +57 36 30.00           ~ 42 0
7 GRB 140817A gB 08 29 03.35 +58 11 24.1           ~ 29 0
8 GRB 141031A gB 08 34 25.96 -59 10 05.8           ~ 34 0
9 GRB 050502B gB 09 30 10.024 +16 59 48.07           ~ 169 0
10 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
11 Fermi bn121217313 gB 10 14 50.32 -62 21 03.3           ~ 69 0
12 GRB 110709B gB 10 58 37.2 -23 27 18           ~ 92 0
13 GRB 141130A gB 14 51 17.28 +47 19 06.3           ~ 24 0
14 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 288 0
15 GRB 060929 gB 17 32 28.920 +29 50 06.20           ~ 60 0
16 GRB 160425A gB 18 41 18.56 -54 21 36.1           ~ 49 0
17 Fermi bn121123421 gB 20 29 16.30 -11 51 35.6           ~ 58 0
18 GRB 110820A gB 22 52 46.10 +70 17 55.3           ~ 39 0
19 GRB 070704 gB 23 38 47.31 +66 15 12.7           ~ 58 0

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