We investigate the dynamics and evolution of merging neutron stars, of neut
ron stars coalescing with stellar-mass black holes, and the formation and p
roperties of accretion tori around the (remnant) black holes.
The three-dimensional Newtonian hydrodynamics equations are integrated by a
Eulerian PPM code on four nested Cartesian grids. The code includes the em
ission and backreaction of gravitational waves as well as a physical nuclea
r equation-of-state [Lattimer & Swesty 1991] and the neutrino emission from
the hot matter. Lepton number and energy losses of the gas due to neutrino
emission are treated by an elaborate neutrino leakage scheme which takes i
nto account neutrinos and antineutrinos of all flavors. Neutrino-antineutri
no annihilation in the vicinity of the merger is evaluated in a post-proces
sing step. The gravity of the black hole is described with a Newtonian or,
alternatively, with a Paczynski-Wiita potential. The hydrodynamic effect of
the black hole is simulated by extracting all matter that flows into a sph
ere with radius equal to the Schwarzschild radius of the black hole or, in
accretion simulations, twice the Schwarzschild radius.
The NS/NS and BH/NS merging models yield information about gravitational wa
ve and neutrino emission. Also, they allow us to determine the physical pro
perties (masses, densities, temperatures, estimated life times) of the remn
ants of the mergers: a black hole surrounded by an accretion torus. In the
NS/NS case, a thick disk with a mass around 0.1M(.) forms after the massive
and very compact central object that contains most of the mass of the merg
ed neutron stars, has collapsed to a black hole, presumably on a dynamical
time scale. The dynamics of BH/NS mergers is very sensitive to the neutron
star to black hole mass ratio. For low ratios the neutron star transfers ma
ss to the black hole during a few cycles of orbital decay and subsequent wi
dening before finally being disrupted, whereas for ratios near unity the ne
utron star is already destroyed during its first approach. A gas mass of ab
out 0.5M(.) is left in an accretion torus around the black hole.
The accretion tori radiate neutrinos at luminosities of up to several 10(53
) erg/s. Higher luminosities are found for larger disk masses and smaller b
lack holes. The emitted neutrinos and antineutrinos annihilate into e(+/-)
pairs with efficiencies of a few percent and rates of up to similar to 2 X
10(52) erg/s, releasing an estimated energy of up to similar to 10(51) erg
in a pair-plasma fireball. The torus geometry favors relativistic expansion
of the pair plasma along the baryon depleted system axis. The occurrence o
f moderately beamed jets with opening angles of several ten degrees is ther
efore likely. The jet energies and short accretion times of the tori of abo
ut 0.1s are in the right range to account for the subclass of short and les
s energetic gamma-ray bursts.