We study the Navier-Stokes equations for compressible barotropic
fluids in a bounded or unbounded domain Ω of R3. We first prove the local existence of solutions
(ρ,u)
in C([0,T∗];(ρ∞+H3(Ω))×(D01∩D3)(Ω)) under the assumption that the data satisfies a natural
compatibility condition. Then deriving the smoothing effect of the
velocity u in t>0, we conclude that (ρ,u) is a classical
solution in (0,T∗∗)×Ω for some T∗∗∈(0,T∗]. For these results, the initial density needs not be bounded
below away from zero and may vanish in an open subset ({\it vacuum})
of Ω