F. Merging neutron stars
Neutron star binary mergers [86, 276] or neutron star - black hole binary mergers [286] (hereafter called mergers) also produce a black hole - accretion disk system and are candidates for the inner engines of GRBs, specifically of short GRBs. These mergers take place because of the decay of the binary orbits due to gravitational radiation emission as was beautifully demonstrated in the famous binary pulsar PSR 1913+16 [405].
These mergers take place at a rate of
10-6 events
per year per galaxy
[278,
300,
414].
This is the rate of merger of binaries of the type of PSR 1913+16
whose life time is or order of several 108 years. Various
population synthesis calculations suggest that there is also
another population of short lived binaries
[18,
297,
410,
411].
These binaries form with very close orbits and hence with short
lifetimes of the order of 105 yrs. Even thought the overall
rate of such mergers could be comparable to those of the
PSR 1913+16 type one cannot expect to catch a binary in our galaxy
in such a stage. Similarly unlike the long lived mergers that may
be kicked from their host galaxy within their long life time
[44,
276]
this short lived population remains within the galaxy when they merge
[18].
Earlier simulations of mergers focused on the gravitational
radiation from this system. Davies et al.
[72]
begun a series of numerical simulation of neutron star merger that
focused on GRB related aspects
[11,
349,
350,
351].
Using a SPH scheme they followed NS mergers under different
assumptions (Newtonian with ad hoc addition of gravitational
radiation back reaction or Post Newtonian), with different
equations of state (adiabatic or realistic) and with different
initial spin axis and mass rations and different estimates of the
effects of neutrino cooling. A parallel set of simulations was
carried out by Janka and Ruffert
[180],
Ruffert and Janka
[354,
355,
356],
Ruffert et al.
[357]
who used particle in cell methods. Both kinds of simulations yield
comparable results. The merger results in a black hole - accretion
disk system. The mass of the accretion disk is of order
0.1M
and it depends, of course somewhat on the orientation
of the spins and the relative masses of the two neutron stars.
A merger releases ~ 5 × 1053 ergs but most of this
energy is in the form of low energy neutrinos and gravitational
waves. Still there is enough energy available to power a GRB but
is not clear how the GRB is produced. A central question is, of
course, how does a merger generate the relativistic wind required
to power a GRB. Eichler et al.
[86]
suggested that about
one thousandth of these neutrinos annihilate and produce pairs
that in turn produce gamma-rays via
e+
e-
. This idea
was criticized on
several grounds by different authors the main problem is that it
does not produce enough energy. For example Jaroszynksi
[181]
pointed out that a large fraction of the
neutrinos will be swallowed by the black hole that forms. An
alternative source of energy within the merger model is the
accretion power of a disk that forms around the black hole. This
brings us back to the canonical black hole - accretion disk scenario.