2018ApJ...869..155S


Query : 2018ApJ...869..155S

2018ApJ...869..155S - Astrophys. J., 869, 155-155 (2018/December-3)

On the magnetar origin of the GRBs presenting X-ray afterglow plateaus.

STRATTA G., DAINOTTI M.G., DALL'OSSO S., HERNANDEZ X. and DE CESARE G.

Abstract (from CDS):

The X-ray afterglow plateau emission observed in many gamma-ray bursts (GRBs) has been interpreted as being fueled either by fallback onto a newly formed black hole or by the spin-down luminosity of an ultra-magnetized millisecond neutron star. If the latter model is assumed, GRB X-ray afterglow light curves can be reproduced analytically. We fit a sample of GRB X-ray plateaus, interestingly yielding a distribution in the diagram of magnetic field versus spin period (B-P) consistent with B ∝ P7/6, which is consistent with GRB expectations of the well-established physics of the spin-up line for accreting Galactic X-ray pulsars. The normalization of the relation that we obtain perfectly matches spin-up line predictions for typical neutron star masses (∼1 M☉) and radii (∼10 km), and for mass accretion rates typically expected in GRBs, 10–4M☉s–1< {dot}M< 10–1M☉s–1. Short GRBs with extended emission (SEEs) appear toward the long-period end of the distribution, and long GRBs (LGRBs) toward the short-period end. This result is consistent with expectations from the spin-up limit, where the total accreted mass determines the position of the neutron star in the B-P diagram. The B-P distributions for LGRBs and SEEs are statistically different, further supporting the idea that the fundamental plane relation-a tri-dimensional correlation between the X-ray luminosity at the end of the plateau, the end time of the plateau, and the 1 s peak luminosity in the prompt emission-is a powerful discriminant among those populations. Our conclusions are robust against suppositions regarding the collimation angle of the GRB and the magnetar braking index, which shift the resulting properties of the magnetar parallel to the spin-up line, and strongly support a magnetar origin for GRBs presenting X-ray plateaus.

Abstract Copyright: © 2018. The American Astronomical Society. All rights reserved.

Journal keyword(s): gamma-ray burst: general - gamma-ray burst: individual - stars: magnetars

Simbad objects: 53

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Number of rows : 53
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 060912A gB 00 21 08.11 +20 58 18.9           ~ 116 1
2 Fermi bn081221681 gB 01 03 10.2 -24 32 53           ~ 186 0
3 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
4 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 217 0
5 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 147 0
6 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
7 GRB 070318 gB 03 13 56.830 -42 56 46.30 18.27 16.23 15.49     ~ 170 0
8 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
9 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
10 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
11 Fermi bn131105087 gB 04 43 53.50 -63 00 17.7           ~ 95 0
12 Fermi bn120907017 gB 04 58 59.99 -09 18 53.7           ~ 89 0
13 GRB 110422A gB 07 28 11.21 +75 06 24.0           ~ 113 0
14 GRB 081028 gB 08 07 34.40 +02 18 16.8           ~ 125 0
15 Fermi bn120118709 gB 08 19 29.05 -07 11 05.1           ~ 87 0
16 Fermi bn140206304 gB 09 41 16.90 +66 45 42.7           ~ 149 0
17 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
18 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
19 GRB 100219A gB 10 16 48.48 -12 34 00.0           ~ 130 0
20 GRB 080430 gB 11 01 14.63 +51 41 07.8           ~ 157 0
21 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
22 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
23 GRB 070810A gB 12 39 51.18 +10 45 02.8           ~ 80 0
24 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 198 0
25 GRB 070208 gB 13 11 32.607 +61 57 54.37 20.79 20.79 19.86     ~ 119 0
26 Fermi bn120811649 gB 13 18 43.82 +62 18 02.8           ~ 113 0
27 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
28 GRB 120521C gB 14 17 09.10 +42 08 39.8           ~ 93 0
29 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 214 0
30 GRB 090205 gB 14 43 40.00 -27 50 51.4           ~ 99 0
31 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 241 0
32 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
33 Fermi bn120922939 gB 15 38 59.67 -20 10 55.0           ~ 88 0
34 GRB 120404A gB 15 40 02.29 +12 53 06.3           ~ 104 0
35 GRB 140903A G 15 52 03.2650 +27 36 10.710           ~ 138 0
36 GRB 070521 gB 16 10 38.600 +30 15 22.70           ~ 164 0
37 GRB 120327A gB 16 27 27.49 -29 24 53.8           ~ 116 0
38 GRB 090418A gB 17 57 15.17 +33 24 21.1           ~ 101 0
39 Fermi bn140506880 gB 18 27 06.04 -55 38 08.7           ~ 113 0
40 GRB 070529 gB 18 54 58.230 +20 39 34.00 20.38   17.25     ~ 98 0
41 Fermi bn140512814 gB 19 17 28.81 -15 05 39.5           ~ 133 0
42 Fermi bn121128212 gB 20 02 23.88 +54 17 59.1           ~ 128 0
43 GRB 070508 gB 20 51 11.810 -78 23 04.88     19.62     ~ 144 0
44 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
45 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 210 0
46 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
47 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
48 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 286 1
49 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
50 GRB 131117A gB 22 09 19.47 -31 45 44.5           ~ 67 0
51 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
52 GRB 081029 gB 23 07 06 -68 10.7           ~ 121 0
53 GRB 061222A gB 23 53 03.419 +46 31 58.60           ~ 177 0

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