2013MNRAS.430.1061R


Query : 2013MNRAS.430.1061R

2013MNRAS.430.1061R - Mon. Not. R. Astron. Soc., 430, 1061-1087 (2013/April-1)

Signatures of magnetar central engines in short GRB light curves.

ROWLINSON A., O'BRIEN P.T., METZGER B.D., TANVIR N.R. and LEVAN A.J.

Abstract (from CDS):

A significant fraction of the long gamma-ray bursts (LGRBs) in the Swift sample have a plateau phase showing evidence of ongoing energy injection. We suggest that many short gamma-ray bursts (SGRBs) detected by the Swift satellite also show evidence of energy injection. Explaining this observation within the typical SGRB progenitor model is challenging as late time accretion, often used to explain plateaus in LGRBs, is likely to be absent from the SGRB population. Alternatively, it is predicted that the remnant of neutron star-neutron star mergers may not collapse immediately to a black hole (or even collapse at all), forming instead an unstable millisecond pulsar (magnetar) which powers a plateau phase in the X-ray light curve.

By fitting the magnetar model to all of the Swift SGRBs observed until 2012 May, we find that about half can be clearly fitted with a magnetar plateau phase while the rest are consistent with forming a magnetar but the data are insufficient to prove a plateau phase. More data, both at early times and a larger sample, are required to confirm this. This model can be tested by detecting the gravitational wave emission from events using the next generation gravitational wave observatories.


Abstract Copyright: © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

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

Simbad objects: 49

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Number of rows : 49
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 070810B gB 00 35 48.4 +08 49 18           ~ 57 0
2 Fermi bn100117879 G 00 45 04.6610 -01 35 42.020           ~ 155 0
3 Fermi bn111117510 gB 00 50 46.220 +23 00 39.22           ~ 141 0
4 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
5 GRB 050911A gB 00 54 38.290 -38 50 58.50           ~ 66 0
6 GRB 100625A gB 01 03 10.98 -39 05 18.3           ~ 124 0
7 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
8 Fermi bn081024245 gB 01 51 33.80 +61 21 08.2           ~ 75 0
9 GRB 070714A gB 02 51 43.36 +30 14 35.1           ~ 63 0
10 GRB 070209 gB 03 04 51.200 -47 22 34.19           ~ 45 0
11 GRB 120305A gB 03 10 08.73 +28 29 30.9           ~ 56 0
12 GRB 050906 gB 03 31 15.28 -14 36 30.1           ~ 76 1
13 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
14 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
15 GRB 060313 G 04 26 28.4020 -10 50 39.901 20.55 21.03 19.66     ~ 156 0
16 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
17 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
18 Fermi bn081101491 gB 06 23 20.70 -00 06 41.5           ~ 39 0
19 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
20 GRB 091109B gB 07 30 59.90 -54 05 30.6           ~ 57 0
21 GRB 051227 gB 08 20 58.107 +31 55 32.01           ~ 127 0
22 GRB 090916 gB 08 26 19.60 +25 56 27.3           ~ 29 0
23 SDSS J093805.33+153719.0 G 09 38 05.33384 +15 37 19.0406           ~ 146 0
24 GRB 120521A gB 09 54 53.91 -49 25 02.4           ~ 41 0
25 GRB 090715A gB 10 08 24.50 +10 00 22.4           ~ 25 0
26 UCAC4 217-047923 * 10 19 02.5992684123 -46 40 11.294771086   13.795 12.458 12.114   ~ 54 0
27 GRB 090515 gB 10 56 41.0 +14 27 22           ~ 122 0
28 SDSS J123612.87+285858.8 BiC 12 36 12.8803407000 +28 58 58.780075656           ~ 328 1
29 GRB 090426 G 12 36 18.0470 +32 59 09.460           ~ 237 0
30 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
31 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
32 GRB 100702A gB 16 22 47.26 -56 31 53.8           ~ 53 0
33 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
34 GRB 090531B gB 16 48 15.0 -36 01 27           ~ 58 0
35 GRB 071112B gB 17 20 51.0 -80 53 02           ~ 50 0
36 GRB 080919 gB 17 40 53.00 -42 22 29.5           ~ 49 0
37 GRB 051105 gB 17 41 09.0 +34 55 15           ~ 11 0
38 GRB 080503 gB 19 06 28.74 +68 47 35.8           ~ 172 0
39 GRB 111020A gB 19 08 12.53 -38 00 43.0           ~ 66 0
40 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
41 GRB 080702A gB 20 52 12.21 +72 18 46.7           ~ 47 0
42 Fermi bn090621922 gB 20 53 49.30 +69 02 02.9           ~ 65 0
43 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
44 GRB 051221 G 21 54 48.626 +16 53 27.16 19.49         ~ 377 0
45 GRB 110112A gB 21 59 43.77 +26 27 24.4           ~ 47 0
46 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 138 0
47 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
48 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
49 GRB 080123 gB 22 35 46.100 -64 54 03.24           ~ 98 0

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