Using an isothermal MHD code, we have performed three-dimensional, high-res
olution simulations of the Parker instability. The initial equilibrium syst
em is composed of exponentially decreasing isothermal gas and a magnetic fi
eld (along the azimuthal direction) under a uniform gravity. The evolution
of the instability can be divided into three phases: linear, nonlinear, and
relaxed. During the linear phase, the perturbations grow exponentially wit
h a preferred scale along the azimuthal direction but with the smallest pos
sible scale along the radial direction, as predicted from linear analyses.
During the nonlinear phase, the growth of the instability is saturated and
flow motion becomes chaotic. Magnetic reconnection occurs, which allows the
gas to cross field lines. This, in turn, results in the redistribution of
the gas and the magnetic field. The system approaches a new equilibrium in
the relaxed phase, which is different from the one seen in two-dimensional
works. The structures formed during the evolution are sheetlike or filament
ary, whose shortest dimension is radial. Their maximum density enhancement
factor relative to the initial value is less than 2. Since the radial dimen
sion is too small and the density enhancement is too low, it is difficult t
o regard the Parker instability alone as a viable mechanism for the formati
on of giant molecular clouds.