We consider a Hamiltonian H which is the sum of a deterministic part H
-0 and of a random potential V. For finite N x N matrices, following a
method introduced by Kazakov, we derive a representation of the corre
lation functions in terms of contour integrals over a finite number of
variables. This allows one to analyse the level correlations, whereas
the standard methods of random matrix theory, such as the method of o
rthogonal polynomials, are not available for such cases. At short dist
ance we recover, for an arbitrary H-0, an oscillating behavior for the
connected two-level correlation.