2018ApJ...855...88D


Query : 2018ApJ...855...88D

2018ApJ...855...88D - Astrophys. J., 855, 88-88 (2018/March-2)

On the origin of supernova-less long gamma-ray bursts.

DADO S. and DAR A.

Abstract (from CDS):

The fraction of long duration gamma-ray bursts (GRBs) without an associated bright supernova (SN-less GRBs) at low redshifts is comparable to that of GRBs associated with bright supernovae (SN-GRBs). The prompt emission and its fast decline phase in both types of GRBs are well described by the cannonball model of GRBs, where inverse Compton scattering of ambient light is the dominant γ-ray production mechanism. However, in SN-less GRBs, the fast decay of the prompt emission appears to be overtaken by an afterglow powered by a millisecond pulsar, while, in SN-GRBs, the late-time X-ray afterglow is well described by synchrotron radiation from the decelerating jet in the interstellar medium. We use their different X-ray light curves to determine the ratio of SN-less GRBs/SN-GRBs at very high redshifts. We find that at z > 4, this ratio is the same as that at small redshifts. Such a z-independent ratio suggests that the origin of SN-less GRBs is a phase transition of neutron stars to quark stars in high-mass X-ray binaries, rather than the merger of neutron stars.

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

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

Simbad objects: 48

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Number of rows : 48
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 050922B gB 00 23 13.400 -05 36 17.80           ~ 73 0
2 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 122 0
3 Fermi bn120729456 gB 00 52 17.84 +49 56 23.1           ~ 96 0
4 GRB 111225A gB 00 52 37.22 +51 34 19.5           ~ 59 0
5 GRB 091018 gB 02 08 46 -57 33.0           ~ 143 0
6 GRB 110918A gB 02 10 09.39 -27 06 19.6           ~ 77 0
7 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 273 1
8 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 940 1
9 Fermi bn120907017 gB 04 58 59.99 -09 18 53.7           ~ 72 0
10 GRB 151027B gB 05 04 52.67 -06 27 00.7           ~ 49 0
11 GRB 100508A gB 05 04 58.99 -20 42 14.1           ~ 35 0
12 GRB 050826 gB 05 51 01.590 -02 38 35.40           ~ 127 0
13 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 107 0
14 GRB 080517 gB 06 48 58.00 +50 44 06.3           ~ 50 1
15 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 287 1
16 GRB 140419A gB 08 27 57.56 +46 14 25.3           ~ 78 0
17 Fermi bn110106893 gB 08 56 37.0 +47 00 10           ~ 72 0
18 Fermi bn141225959 gB 09 15 06.77 +33 47 30.9           ~ 52 0
19 GRB 050505 gB 09 27 03.300 +30 16 23.70     20.74     ~ 191 0
20 GRB 170519A gB 10 53 42.49 +25 22 26.7           ~ 43 0
21 GRB 080430 gB 11 01 14.63 +51 41 07.8           ~ 142 0
22 GRB 060123 gB 11 58 47.83 +45 30 50.9           ~ 44 0
23 SN 2006ag SN* 12 00 17.12 +28 36 22.0       17.9   SNIIn 9 1
24 Fermi bn120521380 gB 13 08 02.33 -52 45 16.6           ~ 31 0
25 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2001 0
26 GRB 140311A gB 13 57 13.29 +00 38 31.7           ~ 69 0
27 SN 2013dx SN* 14 29 14.77 +15 46 26.6           ~ 151 0
28 GRB 090205 gB 14 43 40.00 -27 50 51.4           ~ 85 0
29 Fermi bn160804065 gB 14 46 31.20 +09 59 56.1           ~ 56 0
30 GRB 111005A gB 14 53 15.60 -19 43 19.1           ~ 64 0
31 GRB 140518A gB 15 09 00.60 +42 25 05.6           ~ 53 0
32 GRB 140614A gB 15 24 40.69 -79 07 43.8           ~ 33 0
33 GRB 090814A gB 15 58 26.44 +25 37 52.4           ~ 50 0
34 GRB 130606A gB 16 37 35.12 +29 47 46.4           ~ 154 0
35 GRB 091003A gB 16 46 04.680 +36 37 31.08           ~ 121 0
36 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 180 0
37 GRB 050814 gB 17 36 45.390 +46 20 21.60           ~ 152 0
38 Fermi bn151027166 gB 18 09 56.87 +61 21 12.3           ~ 111 0
39 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1821 2
40 GRB 160623A gB 21 01 11.54 +42 13 15.5           ~ 59 0
41 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 184 0
42 GRB 060614 gB 21 23 32.140 -53 01 36.10 18.89 20.12 19.54     ~ 612 1
43 GRB 060927A gB 21 58 11.930 +05 21 50.32           ~ 196 0
44 GRB 060505 gB 22 07 03.440 -27 48 51.89           ~ 259 1
45 Fermi bn080916406 gB 22 25 09.30 -57 01 33.7           ~ 157 0
46 GRB 061110A gB 22 25 09.800 -02 15 30.70 21.43         ~ 126 0
47 GRB 051109B gB 23 01 50.330 +38 40 46.51           ~ 85 0
48 GRB 051022A gB 23 56 04.200 +19 36 32.30           ~ 187 1

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