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Nowadays the most accounted models for the GRB progenitors can be
divided into two classes: the first includes the core collaps of very
massive stars (``collapsar'' or ``hypernova'' models, [Woosley, 1993],
[Paczynski, 1998]), and
the ``supranova'' model, concerning the formation of a BH from a rapidly
spinning and decelerating NS, left over by a previous SN explosion
([Vietri & Stella, 1998]); the second class includes mergers of compact stars
(NS, BH, or even white dwarfs, provided that at least one mergee
is either a NS or a BH; see [Eichler et al., 1989], [Belczynski et al., 2001]).
Among the remaining models, here we only cite the cannonball model
proposed by Dado, Dar & De Rújula, 2001, which reproduces all the light curves of
the afterglows in association with underlying SNe, that up to now seem
to agree with observations.
The ``collapsar'' model deals with a rotating massive star, whose
Fe core collapses, producing a Kerr BH surrounded by a
torus, whose matter is accreted at a very high rate; the energy
can be extracted in two ways: first, by accretion of the disk matter
by the BH; second, from the rotational energy of the BH via the
Blandford-Znajek process ([Blandford & Znajek, 1977]).
The so released energy amounts to
ergs; according
to this model, a fireball with a luminosity
300 times greater
than that of a normal SN is produced. In this case, the GRB would be
produced in a dense environment, near star forming regions.
The ``supranova model'' requires a supra-massive NS, which is
rapidly spinning down, untill it implodes to a BH; during
this implosion the surrounding matter, previously produced
by the SN explosion, is swept up, leading to a baryon-clean
environment. The presence of a
torus is
predicted, while the energy extraction occurs via the conversion
of the Poynting flux into a magnetized relativistic wind.
Finally, the merging of compact stars, like in the NS-NS case,
has the following characteristics: since their typical life
should be of the order of
years, and given that
such systems usually have large escape velocities, they
are likely to be found away from star forming regions.
Figure:
GRB-Host Galaxy Offset Distribution. It seems to
favour a progenitor population associated with star forming
regions. (From [Djorgovski et al., 2001]).
 |
In particular, this property does not seem to agree with the observed
distribution of GRB-host galaxy offsets (fig.
):
this looks like following the light of their hosts, that is
roughly proportional to the density of star formation
(especially for the high-
galaxies).
However, this piece of evidence does not suffice for
discarding this model yet.
The result of such a merging is a Kerr BH, with an energy
release of
ergs. Also in this case, it is
possible that a
accretion disk is
formed and that is accreted within a few dozen seconds,
then producing the internal shocks responsible for the burst.
Eventually, it is worth mentioning that it has been suggested
that the short duration bursts might be produced by such
compact binary systems.
Next: Rapid Localizations of Bursts
Up: Theoretical Models
Previous: The Fireball Model
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Cristiano Guidorzi
2003-07-31