  We consider fermions in one-dimensional superlattices (SL's), modeled by
site-dependent Hubbard-U couplings arranged in a repeated pattern of repulsive
(i.e., U>0) and free (U=0) sites. Density Matrix Renormalization Group (DMRG)
diagonalization of finite systems is used to calculate the local moment and the
magnetic structure factor in the ground state. We have found four regimes for
magnetic behavior: uniform local moments forming a spin-density wave (SDW),
`floppy' local moments with short-ranged correlations, local moments on
repulsive sites forming long-period SDW's superimposed with short-ranged
correlations, and local moments on repulsive sites solely with long-period
SDW's; the boundaries between these regimes depend on the range of electronic
densities, rho, and on the SL aspect ratio. Above a critical electronic
density, rho_{uparrow downarrow}, the SDW period oscillates both with rho and
with the spacer thickness. The former oscillation allows one to reproduce all
SDW wave vectors within a small range of electronic densities, unlike the
homogeneous system. The latter oscillation is related to the exchange
oscillation observed in magnetic multilayers. A crossover between regimes of
`thin' to `thick' layers has also been observed.
