2019ApJ...877..153Z

Query : 2019ApJ...877..153Z

2019ApJ...877..153Z - Astrophys. J., 877, 153-153 (2019/June-1)

Magnetar as central engine of Gamma-ray bursts: central engine-jet connection, wind-jet energy partition, and origin of some ultra-long bursts.

ZOU L., ZHOU Z.-M., XIE L., ZHANG L.-L., LU H.-J., ZHONG S.-Q., WANG Z.-J. and LIANG E.-W.

Abstract (from CDS):

Gamma-ray bursts (GRBs) central engines and jet production mechanisms are still open questions. Assuming that the shallow decay segments of canonical X-ray afterglow light curves of Swift GRBs are attributed to the magnetic dipole (MD) radiations of newly born magnetars, we derive the parameters of the magnetars and explore their possible relations to jet and MD wind emission. We show that the magnetar initial spin period (P0) are tightly correlated with the jet energy (Ejet), which is almost proportional to the wind energy (Ewind). Our least-squares fits yield P0∝Ejet^-0.36±0.03^ and Ewind∝Ejet^0.91±0.07^. These relations may imply that a magnetar with faster rotating speed can power a more energetic GRB, and energy partition between the jet and wind may be quasi-universal. Although the P0-Ejet relation is driven by a few sub-energetic GRBs in our sample, our Monte Carlo simulation analysis shows that sample selection biases from instrumental flux limits and contaminations of the bright jet afterglows cannot make this correlation. Within this jet-wind paradigm, we propose that GRB 101225A-like ultra-long GRBs, whose prompt gamma-ray/X-ray light curves are featured as a long-lasting plateau with a sharp drop, may be the orphan MD wind emission being due to misalignment of their jet axis to the light of sight. We briefly discuss the orphan MD wind emission and its association with the gravitational-wave radiation of newly born magnetars.

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

Journal keyword(s): gamma-ray burst: general - gamma-ray burst: individual: (GRB 101225A, GRB 170714A) - methods: statistical

Simbad objects: 128

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Number of rows : 128
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 101225A gB 00 00 47.48 +44 36 01.0           ~ 163 0
2 GRB 070110 gB 00 03 39.270 -52 58 27.00 21.8 21.9 21.2     ~ 220 0
3 GRB 110420A gB 00 08 39.27 -37 53 11.9           ~ 33 0
4 GRB 150910A gB 00 22 40.14 +33 28 22.4           ~ 79 0
5 Fermi bn100522157 gB 00 27 56.79 +09 24 06.6           ~ 57 0
6 GRB 170607A gB 00 29 27.84 +09 14 35.5           ~ 62 0
7 GRB 180115A gB 00 48 09.31 -15 37 50.5           ~ 28 0
8 Fermi bn140703026 gB 00 51 58.99 +45 06 05.4           ~ 90 0
9 GRB 160607A gB 00 54 40.16 -04 56 54.5           ~ 22 0
10 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
11 GRB 081128 gB 01 23 12.98 +38 07 37.5           ~ 42 0
12 Fermi bn100814160 gB 01 29 53.61 -17 59 43.6           ~ 219 0
13 GRB 100901A gB 01 49 03.56 +22 45 30.6           ~ 170 0
14 GRB 100906A gB 01 54 44.19 +55 37 49.8           ~ 233 0
15 GRB 090728 gB 01 58 35 +41 37.9           ~ 32 0
16 GRB 070616 gB 02 08 36.430 +56 56 44.91           ~ 79 0
17 GRB 091018 gB 02 08 46 -57 33.0           ~ 169 0
18 GRB 170714A gB 02 17 17 +01 58.0           ~ 50 0
19 GRB 060202 gB 02 23 22.940 +38 23 03.70           ~ 102 0
20 GRB 070129 gB 02 28 00.940 +11 41 04.00       21.3   ~ 120 0
21 GRB 140916A gB 02 41 35.88 -39 41 11.2           ~ 22 0
22 Fermi bn130925164 gB 02 44 42.38 -26 09 15.8           ~ 184 0
23 Fermi bn110213220 gB 02 51 51.37 +49 16 21.2           ~ 175 0
24 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
25 GRB 050822 gB 03 24 27.240 -46 01 59.20     20.82     ~ 115 0
26 Fermi bn130609902 gB 03 35 05.11 -40 10 26.7           ~ 54 0
27 GRB 110808A gB 03 49 04.28 -44 11 40.3           ~ 64 0
28 GRB 060211A gB 03 53 32.600 +21 29 19.20           ~ 53 0
29 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
30 GRB 111008A gB 04 01 48.220 -32 42 34.09           ~ 127 0
31 Fermi bn170113420 gB 04 06 59 -71 56.0           ~ 64 0
32 GRB 121027A gB 04 14 23.450 -58 49 47.17           ~ 136 0
33 GRB 070328 gB 04 20 27.680 -34 04 00.60 20.29         ~ 97 0
34 Fermi bn101024486 gB 04 26 01.24 -77 15 55.1           ~ 54 0
35 GRB 090407 gB 04 35 54.98 -12 40 45.5           ~ 87 0
36 GRB 100508A gB 05 04 58.99 -20 42 14.1           ~ 39 0
37 GRB 180329B gB 05 31 36.91 -23 41 27.4           ~ 49 0
38 GRB 050826 gB 05 51 01.590 -02 38 35.40           ~ 136 0
39 GRB 170317A gB 06 12 20 +50 30.0           ~ 30 0
40 GRB 141017A gB 06 14 31.18 -58 34 56.5           ~ 26 0
41 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
42 GRB 060510A gB 06 23 27.980 -01 09 46.20 18.19   18.45     ~ 58 0
43 GRB 090904A gB 06 43 32.35 +50 12 10.8           ~ 43 0
44 GRB 061202 gB 07 02 06.190 -74 41 54.91           ~ 83 0
45 GRB 150626A gB 07 25 20.84 -37 46 50.4           ~ 21 0
46 GRB 070420 gB 08 04 55.170 -45 33 19.99 20.39 20.01 17.16     ~ 83 0
47 GRB 141121A gB 08 10 40.68 +22 13 02.7           ~ 108 0
48 GRB 060428A gB 08 14 10.840 -37 10 11.70     19.97     ~ 54 0
49 Fermi bn120118709 gB 08 19 29.05 -07 11 05.1           ~ 87 0
50 GRB 141031A gB 08 34 25.96 -59 10 05.8           ~ 34 0
51 GRB 051016B gB 08 48 27.810 +13 39 20.00 20.45         ~ 153 0
52 Fermi bn100704149 gB 08 54 33.92 -24 12 09.7           ~ 103 0
53 SN 2012bz SN* 09 07 38.38 +14 01 07.5           SNIb/c 193 1
54 Fermi bn090516353 gB 09 12 59 -11 50.9           ~ 173 0
55 GRB 160327A gB 09 46 48.56 +54 00 46.4           ~ 43 0
56 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
57 GRB 070306 gB 09 52 23.220 +10 28 55.20           ~ 222 1
58 GRB 171222A gB 09 53 06.69 +35 37 36.1           ~ 57 0
59 GRB 060602 gB 09 58 16.730 +00 18 12.70           ~ 8 0
60 GRB 060602A gB 09 58 16.93 +00 18 12.8           ~ 49 0
61 Fermi bn111228657 gB 10 00 16.04 +18 17 52.2           ~ 201 0
62 GRB 170202A gB 10 10 06 +05 01.0           ~ 90 0
63 Fermi bn121217313 gB 10 14 50.32 -62 21 03.3           ~ 69 0
64 GRB 050319 gB 10 16 47.900 +43 32 53.80   18.02 17.01     ~ 274 0
65 GRB 130315A gB 10 30 09.90 -51 47 37.4           ~ 26 0
66 Fermi bn171120556 gB 10 55 09.80 +22 27 29.6           ~ 34 0
67 GRB 080430 gB 11 01 14.63 +51 41 07.8           ~ 157 0
68 SN 2017iuk SN* 11 09 39.49 -12 35 18.7           SNII 210 0
69 GRB 100305A gB 11 13 28.06 +42 24 14.1           ~ 34 0
70 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
71 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
72 Fermi bn100615083 gB 11 48 49.25 -19 28 52.2           ~ 133 0
73 GRB 060712 gB 12 16 16.170 +35 32 17.70           ~ 38 0
74 GRB 140114A gB 12 34 05.10 +27 57 02.6           ~ 61 0
75 GRB 100302A gB 13 02 03.66 +74 35 22.5           ~ 83 0
76 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
77 GRB 160630A gB 13 13 02.19 -56 02 30.6           ~ 20 0
78 Fermi bn120811649 gB 13 18 43.82 +62 18 02.8           ~ 113 0
79 GRB 091130B gB 13 32 35.62 +34 05 18.8           ~ 39 0
80 GRB 060204B gB 14 07 14.900 +27 40 36.40           ~ 93 0
81 GRB 090529 gB 14 09 52.49 +24 27 33.5           ~ 89 0
82 GRB 120521C gB 14 17 09.10 +42 08 39.8           ~ 93 0
83 GRB 120308A gB 14 36 20.02 +79 41 12.0           ~ 79 0
84 GRB 050915B gB 14 36 25.890 -67 24 33.21           ~ 56 0
85 GRB 050802 gB 14 37 05.820 +27 47 12.62 16.85 17.38 16.97     ~ 186 0
86 GRB 080310 gB 14 40 13.89 -00 10 30.4           ~ 214 0
87 GRB 060814 gB 14 45 21.480 +20 35 11.80           ~ 241 0
88 Fermi bn090813174 gB 15 00 15.60 +88 34 15.8           ~ 62 0
89 GRB 140518A gB 15 09 00.60 +42 25 05.6           ~ 68 0
90 GRB 060714 gB 15 11 26.450 -06 33 58.30   20.21 18.54     ~ 209 0
91 GRB 080229 gB 15 12 52.31 -14 42 16.2           ~ 68 0
92 GRB 090404 gB 15 56 55.80 +35 31 03.4           ~ 79 0
93 GRB 060502A gB 16 03 42.480 +66 36 02.49     18.65     ~ 143 0
94 GRB 060219 gB 16 07 21.520 +32 18 57.59           ~ 50 0
95 GRB 070521 gB 16 10 38.600 +30 15 22.70           ~ 164 0
96 Fermi bn110102788 gB 16 23 31.41 +07 36 49.8           ~ 62 0
97 GRB 060807 gB 16 50 02.600 +31 35 30.70           ~ 61 0
98 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
99 GRB 100614A gB 17 34 08.20 +49 13 56.4           ~ 45 0
100 GRB 050814 gB 17 36 45.390 +46 20 21.60           ~ 166 0
101 Fermi bn140818781 gB 18 04 32.53 -01 23 10.6           ~ 24 0
102 Fermi bn151027166 gB 18 09 56.87 +61 21 12.3           ~ 143 0
103 GRB 060109 gB 18 50 43.650 +31 59 26.40           ~ 52 0
104 Fermi bn140512814 gB 19 17 28.81 -15 05 39.5           ~ 133 0
105 Fermi bn100725475 gB 19 20 07 +76 57.3           ~ 55 0
106 GRB 120324A gB 19 24 18.84 +24 07 46.4           ~ 45 0
107 GRB 150428B gB 19 30 33.46 +04 07 31.8           ~ 23 0
108 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
109 GRB 100425A gB 19 56 47.16 -26 25 50.5           ~ 91 0
110 Fermi bn080905705 gB 20 06 57.93 -62 33 46.8           ~ 119 0
111 Fermi bn140709051 gB 20 18 38.96 +51 13 29.9           ~ 43 0
112 GRB 050315 gB 20 25 54.100 -42 36 02.19           ~ 225 0
113 GRB 050713B gB 20 31 15.570 +60 56 43.70           ~ 72 0
114 GRB 160625B gB 20 34 23.67 +06 55 11.1           ~ 235 0
115 GRB 070508 gB 20 51 11.810 -78 23 04.88     19.62     ~ 144 0
116 GRB 090727 gB 21 03 50.79 +64 55 29.8           ~ 39 0
117 GRB 050713A gB 21 22 09.530 +77 04 29.50           ~ 125 0
118 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
119 GRB 161117A gB 21 28 12.59 -29 36 49.9           ~ 74 0
120 GRB 060605 gB 21 28 37.320 -06 03 31.30   20.12 16.53     ~ 210 0
121 Fermi bn081126899 gB 21 34 03.54 +48 42 35.2           ~ 76 0
122 GRB 060607 gB 21 58 50.400 -22 29 46.70 18.49 16.67 15.09     ~ 318 0
123 GRB 060604 gB 22 28 55.010 -10 54 55.80 20.34 20.31       ~ 134 0
124 GRB 110820A gB 22 52 46.10 +70 17 55.3           ~ 39 0
125 GRB 081029 gB 23 07 06 -68 10.7           ~ 121 0
126 Fermi bn180411519 gB 23 47 25.09 +66 46 41.6           ~ 17 0
127 Fermi bn140323433 gB 23 47 50.31 -79 54 16.4           ~ 36 0
128 GRB 061222A gB 23 53 03.419 +46 31 58.60           ~ 177 0

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