We examine in full generality the phase behavior of systems whose constitue
nt particles interact by means of potentials that do not diverge at the ori
gin, are free of attractive parts, and decay fast enough to zero as the int
erparticle separation r goes to infinity. By employing a mean field-density
functional theory which is shown to become exact at high temperatures and/
or densities, we establish a criterion that determines whether a given syst
em will freeze at all temperatures or it will display reentrant melting and
an upper freezing temperature.