2014ApJ...785...74L


Query : 2014ApJ...785...74L

2014ApJ...785...74L - Astrophys. J., 785, 74 (2014/April-2)

A test of the millisecond magnetar central engine model of gamma-ray bursts with Swift data.

LU H.-J. and ZHANG B.

Abstract (from CDS):

A rapidly spinning, strongly magnetized neutron star (magnetar) has been proposed as one possible candidate of the central engine of gamma-ray bursts (GRBs). We systematically analyze the Swift/XRT light curves of long GRBs detected before 2013 August, and characterize them into four categories based on how likely they may harbor a magnetar central engine: Gold, Silver, Aluminum, and Non-magnetar. We also independently analyze the data of short GRBs with a putative magnetar central engine. We then perform a statistical study of various properties of the magnetar samples and the non-magnetar sample, and investigate whether the data are consistent with the hypothesis that there exist two types of central engines. By deriving the physical parameters of the putative magnetars, we find that the observations of the Gold and Silver samples are generally consistent with the predictions of the magnetar model. For a reasonable beaming factor for long GRBs, the derived magnetar surface magnetic field Bp and initial spin period P0 fall into the reasonable range. Magnetar winds in short GRBs, on the other hand, are consistent with being isotropic. No GRB in the magnetar sample has a beam-corrected total energy exceeding the maximum energy budget defined by the initial spin energy of the magnetar, while some non-magnetar GRBs do violate such a limit. With beaming correction, on average the non-magnetar sample is more energetic and luminous than the magnetar samples. Our analysis hints that millisecond magnetars are likely operating in a good fraction, but probably not all, GRBs.

Abstract Copyright:

Journal keyword(s): gamma rays: general - methods: statistical - radiation mechanisms: non-thermal

Simbad objects: 56

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Number of rows : 56
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 GRB 070110 gB 00 03 39.270 -52 58 27.00 21.8 21.9 21.2     ~ 202 0
2 Fermi bn081221681 gB 01 03 10.2 -24 32 53           ~ 159 0
3 Fermi bn091208410 gB 01 57 38.50 +16 52 50.7           ~ 193 0
4 GRB 060908 gB 02 07 18.360 +00 20 31.20 16.99 18.34 16.85     ~ 200 0
5 GRB 070616 gB 02 08 36.430 +56 56 44.91           ~ 75 0
6 GRB 060202 gB 02 23 22.940 +38 23 03.70           ~ 95 0
7 GRB 060906 gB 02 43 00.900 +30 21 42.12     19.84     ~ 133 0
8 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 291 1
9 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 104 0
10 GRB 121027A gB 04 14 23.450 -58 49 47.17           ~ 114 0
11 GRB 121024A gB 04 41 53.31 -12 17 26.1           ~ 121 0
12 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 130 0
13 GRB 970228 gB 05 01 46.7 +11 46 53           ~ 638 1
14 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 283 0
15 GRB 070420 gB 08 04 55.170 -45 33 19.99 20.39 20.01 17.16     ~ 80 0
16 GRB 081028 gB 08 07 34.40 +02 18 16.8           ~ 110 0
17 SN 2012bz SN* 09 07 38.38 +14 01 07.5           SNIb/c 164 1
18 GRB 050505 gB 09 27 03.300 +30 16 23.70     20.74     ~ 192 0
19 GRB 060108 gB 09 48 01.980 +31 55 08.59           ~ 102 0
20 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 207 1
21 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 359 0
22 Fermi bn111228657 gB 10 00 16.04 +18 17 52.2           ~ 167 0
23 GRB 080430 gB 11 01 14.63 +51 41 07.8           ~ 143 0
24 GRB 130603B gB 11 28 48.16 +17 04 18.2           ~ 351 0
25 GRB 090426 gB 12 36 19.49 +32 59 05.5           ~ 206 0
26 GRB 121229A gB 12 40 23.41 -50 35 37.2           ~ 51 0
27 GRB 100724A gB 12 58 10.38 -11 06 09.3           ~ 162 0
28 GRB 080607A gB 12 59 47.14 +15 55 09.6           ~ 235 0
29 GRB 090419 gB 13 07 42.95 -75 36 21.1           ~ 23 0
30 GRB 070809 gB 13 35 04.2 -22 07 07           ~ 156 0
31 GRB 060801 gB 14 12 01.290 +16 58 54.00           ~ 158 0
32 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 165 0
33 GRB 060526 gB 15 31 18.360 +00 17 04.90   18.31 17.16     ~ 270 0
34 GRB 081203A gB 15 32 07.6 +63 31 15           ~ 159 0
35 GRB 050401 gB 16 31 28.84 +02 11 14.5           ~ 336 0
36 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 181 0
37 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 178 0
38 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 199 0
39 GRB 070529 gB 18 54 58.230 +20 39 34.00 20.38   17.25     ~ 89 0
40 GRB 060413 gB 19 25 07.850 +13 45 29.90           ~ 66 0
41 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 322 0
42 Fermi bn121128212 gB 20 02 23.88 +54 17 59.1           ~ 105 0
43 GRB 120213A gB 20 04 02.83 +65 24 40.6           ~ 31 0
44 Fermi bn080905705 gB 20 06 57.93 -62 33 46.8           ~ 103 0
45 GRB 130102A gB 20 45 41.63 +49 49 03.5           ~ 21 0
46 GRB 060614 gB 21 23 32.140 -53 01 36.10 18.89 20.12 19.54     ~ 619 1
47 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 194 0
48 GRB 060522 gB 21 31 44.850 +02 53 10.80           ~ 131 0
49 GRB 051221 gB 21 54 48.626 +16 53 27.16 19.49         ~ 353 1
50 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 296 0
51 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 188 0
52 GRB 090510 gB 22 14 12.60 -26 35 51.1           ~ 496 1
53 GRB 061110A gB 22 25 09.800 -02 15 30.70 21.43         ~ 127 0
54 GRB 060604 gB 22 28 55.010 -10 54 55.80 20.34 20.31       ~ 126 0
55 Fermi bn090927422 gB 22 55 53.41 -70 58 49.3           ~ 95 0
56 GRB 050803 gB 23 22 37.910 +05 47 09.00           ~ 117 0

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