2019ApJ...878...62X


Query : 2019ApJ...878...62X

2019ApJ...878...62X - Astrophys. J., 878, 62-62 (2019/June-2)

Determining the efficiency of converting magnetar spindown energy into gamma-ray burst X-ray afterglow emission and its possible implications.

XIAO D. and DAI Z.-G.

Abstract (from CDS):

Plateaus are common in X-ray afterglows of gamma-ray bursts. Among the few scenarios regarding their origin, the leading one is that there exists a magnetar inside and it persistently injects its spindown energy into an afterglow. In previous studies, the radiation efficiency of this process is assumed to be a constant at >=0.1, which is quite simple and strong. In this work we obtain the efficiency from a physical point of view and find that this efficiency strongly depends on the injected luminosity. One implication of this result is that those X-ray afterglow light curves that show steeper temporal decay than t–2 after the plateau phase can be naturally understood now. Also, the braking indexes deduced from afterglow fitting are found to be larger than those in previous studies, which are more reasonable for newborn magnetars.

Abstract Copyright: © 2019. The American Astronomical Society. All rights reserved.

Journal keyword(s): gamma-ray burst: general - radiation mechanisms: general - stars: neutron

Simbad objects: 46

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Number of rows : 46
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 150910A gB 00 22 40.14 +33 28 22.4           ~ 79 0
2 GRB 050922B gB 00 23 13.400 -05 36 17.80           ~ 79 0
3 GRB 170607A gB 00 29 27.84 +09 14 35.5           ~ 62 0
4 Fermi bn140703026 gB 00 51 58.99 +45 06 05.4           ~ 90 0
5 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
6 GRB 091018 gB 02 08 46 -57 33.0           ~ 169 0
7 GRB 070129 gB 02 28 00.940 +11 41 04.00       21.3   ~ 120 0
8 GRB 050822 gB 03 24 27.240 -46 01 59.20     20.82     ~ 115 0
9 Fermi bn130609902 gB 03 35 05.11 -40 10 26.7           ~ 54 0
10 GRB 110808A gB 03 49 04.28 -44 11 40.3           ~ 64 0
11 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
12 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
13 Fermi bn170113420 gB 04 06 59 -71 56.0           ~ 64 0
14 GRB 070328 gB 04 20 27.680 -34 04 00.60 20.29         ~ 97 0
15 GRB 081210 gB 04 41 56.19 -11 15 27.8           ~ 56 0
16 Fermi bn131105087 gB 04 43 53.50 -63 00 17.7           ~ 95 0
17 GRB 180329B gB 05 31 36.91 -23 41 27.4           ~ 49 0
18 GRB 180404A gB 05 34 11.73 -37 10 04.8           ~ 26 0
19 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
20 GRB 140430A gB 06 51 44.58 +23 01 25.5           ~ 81 0
21 GRB 051016B gB 08 48 27.810 +13 39 20.00 20.45         ~ 153 0
22 SN 2012bz SN* 09 07 38.38 +14 01 07.5           SNIb/c 193 1
23 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
24 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
25 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
26 GRB 171222A gB 09 53 06.69 +35 37 36.1           ~ 57 0
27 Fermi bn111228657 gB 10 00 16.04 +18 17 52.2           ~ 201 0
28 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
29 GRB 180325A gB 10 29 42.57 +24 27 48.7           ~ 85 0
30 GRB 170519A gB 10 53 42.49 +25 22 26.7           ~ 55 0
31 GRB 080430 gB 11 01 14.63 +51 41 07.8           ~ 157 0
32 Fermi bn100615083 gB 11 48 49.25 -19 28 52.2           ~ 133 0
33 Fermi bn170705115 gB 12 49 +17.9           ~ 66 0
34 GRB 160227A gB 12 59 13.71 +78 40 45.1           ~ 69 0
35 GRB 100302A gB 13 02 03.66 +74 35 22.5           ~ 83 0
36 GRB 090529 gB 14 09 52.49 +24 27 33.5           ~ 89 0
37 GRB 120521C gB 14 17 09.10 +42 08 39.8           ~ 93 0
38 Fermi bn160804065 gB 14 46 31.20 +09 59 56.1           ~ 79 0
39 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
40 GRB 090404 gB 15 56 55.80 +35 31 03.4           ~ 79 0
41 GRB 170531B gB 19 07 31.99 -16 25 09.3           ~ 38 0
42 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
43 GRB 070508 gB 20 51 11.810 -78 23 04.88     19.62     ~ 144 0
44 GRB 161117A gB 21 28 12.59 -29 36 49.9           ~ 74 0
45 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 210 0
46 GRB 060604 gB 22 28 55.010 -10 54 55.80 20.34 20.31       ~ 134 0

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