2018ApJ...862..130L


Query : 2018ApJ...862..130L

2018ApJ...862..130L - Astrophys. J., 862, 130-130 (2018/August-1)

Gamma-ray Burst/Supernova associations: energy partition and the case of a magnetar central engine.

LU H.-J., LAN L., ZHANG B., LIANG E.-W., KANN D.A., DU S.-S. and SHEN J.

Abstract (from CDS):

The favored progenitor model for Gamma-ray Bursts (GRBs) with Supernova (SN) association is the core collapse of massive stars. One possible outcome of such a collapse is a rapidly spinning, strongly magnetized neutron star ("magnetar"). We systematically analyze the multi-wavelength data of GRB/SN associations detected by several instruments before 2017 June. Twenty GRB/SN systems have been confirmed via direct spectroscopic evidence or a clear light curve bump, as well as some spectroscopic evidence resembling a GRB-SN. We derive/collect the basic physical parameters of the GRBs and the SNe, and look for correlations among these parameters. We find that the peak brightness, 56Ni mass, and explosion energy of SNe associated with GRBs are statistically higher than other Type Ib/c SNe. A statistically significant relation between the peak energy of GRBs and the peak brightness of their associated SNe is confirmed. No significant correlations are found between the GRB energies (either isotropic or beaming-corrected) and the supernova energy. We investigate the energy partition within these systems and find that the beaming-corrected GRB energy of most systems is smaller than the SN energy, with less than 30% of the total energy distributed in the relativistic jet. The total energy of the systems is typically smaller than the maximum available energy of a millisecond magnetar (2 x 1052 erg), especially if aspherical SN explosions are considered. The data are consistent with-although not proof of-the hypothesis that most, but not all, GRB/SN systems are powered by millisecond magnetars.

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

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

Simbad objects: 22

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Number of rows : 22
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 SN 2010ma SN* 00 48 55.35 -34 33 59.5           SNIc 190 1
2 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
3 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
4 SN 2013ez SN* 02 53 56.70 +13 23 13.6           ~ 118 0
5 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
6 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 140 0
7 GRB 080109 gB 06 31 29.0 +70 37 14           ~ 36 0
8 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 336 1
9 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
10 SN 2002lt SN* 08 08 59.858 +06 43 37.52           SNIc: 363 1
11 SN 2012bz SN* 09 07 38.38 +14 01 07.5           SNIb/c 193 1
12 SN 2008D SN* 09 09 30.625 +33 08 20.16     17.5     SNIb 458 1
13 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
14 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
15 GRB 011121 gB 11 34 26.67 -76 01 41.6       23.0   ~ 286 1
16 SN 2013dx SN* 14 29 14.77 +15 46 26.6           ~ 178 0
17 SN 2005nc SN* 18 32 32.560 +26 20 22.34           SNIc: 400 1
18 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
19 iPTF 14bfu SN* 21 52 30.00 +32 00 52.5           SNIc 80 0
20 ASASSN -15lh ev 22 02 15.4 -61 39 34           ~ 187 1
21 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
22 SN 2013fu SN* 23 54 29.91 +29 25 47.6           SNIb/c 144 1

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