2014ApJ...793L..36F


Query : 2014ApJ...793L..36F

2014ApJ...793L..36F - Astrophys. J., 793, L36 (2014/October-1)

Hypercritical accretion, induced gravitational collapse, and binary-driven hypernovae.

FRYER C.L., RUEDA J.A. and RUFFINI R.

Abstract (from CDS):

The induced gravitational collapse (IGC) paradigm has been successfully applied to the explanation of the concomitance of gamma-ray bursts (GRBs) with supernovae (SNe) Ic. The progenitor is a tight binary system composed of a carbon-oxygen (CO) core and a neutron star (NS) companion. The explosion of the SN leads to hypercritical accretion onto the NS companion, which reaches the critical mass, hence inducing its gravitational collapse to a black hole (BH) with consequent emission of the GRB. The first estimates of this process were based on a simplified model of the binary parameters and the Bondi-Hoyle-Lyttleton accretion rate. We present here the first full numerical simulations of the IGC phenomenon. We simulate the core-collapse and SN explosion of CO stars to obtain the density and ejection velocity of the SN ejecta. We follow the hydrodynamic evolution of the accreting material falling into the Bondi-Hoyle surface of the NS all the way up to its incorporation in the NS surface. The simulations go up to BH formation when the NS reaches the critical mass. For appropriate binary parameters, the IGC occurs in short timescales ∼102-103 s owing to the combined effective action of the photon trapping and the neutrino cooling near the NS surface. We also show that the IGC scenario leads to a natural explanation for why GRBs are associated only with SNe Ic with totally absent or very little helium.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: general - stars: black holes - stars: neutron - supernovae: general

Simbad objects: 16

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Number of rows : 16
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 GRB 060202 gB 02 23 22.940 +38 23 03.70           ~ 102 0
3 GRB 061007 gB 03 05 19.510 -50 30 02.50 14.28 14.40 12.95     ~ 315 1
4 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
5 GRB 060729 gB 06 21 31.850 -62 22 12.69           ~ 303 0
6 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 336 1
7 SN 2012bz SN* 09 07 38.38 +14 01 07.5           SNIb/c 193 1
8 GRB 061121 gB 09 48 54.570 -13 11 42.68 17.19 17.71 17.02     ~ 350 0
9 Fermi bn090423330 gB 09 55 33.19 +18 08 57.7           ~ 392 0
10 SN 2013cq SN* 11 32 32.84 +27 41 56.2           SNIc 613 1
11 GRB 090424 gB 12 38 07.40 +16 49 45.9           ~ 269 0
12 GRB 060418 gB 15 45 42.600 -03 38 20.00 15.73 16.19 14.98     ~ 389 0
13 GRB 100418A gB 17 05 26.96 +11 27 41.9           ~ 198 0
14 GRB 090618 gB 19 36 01.80 +78 21 07.1           ~ 358 0
15 GRB 100621A gB 21 01 13.12 -51 06 22.5           ~ 204 0
16 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1

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