  The localization properties of electrons moving in a plane perpendicular to a
spatially-correlated static magnetic field of random amplitude and vanishing
mean are investigated. We apply the method of level statistics to the
eigenvalues and perform a multifractal analysis for the eigenstates. From the
size and disorder dependence of the variance of the nearest neighbor energy
spacing distribution, $P_{W,L}(s)$, a single branch scaling curve is obtained.
Contrary to a recent claim, we find no metal-insulator-transition in the
presence of diagonal disorder. Instead, as in the uncorrelated random magnetic
field case, conventional unitary behavior (all states are localized) is
observed. The eigenstates at the band center, which in the absence of diagonal
disorder are believed to belong to the chiral unitary symmetry class, are shown
to exhibit a $f(\alpha)$-distribution for not too weak random fields. The
corresponding generalized multifractal dimensions are calculated and found to
be different from the results known for a QHE-system.
