  The exact solution of the Dorokhov-Mello-Pereyra-Kumar-equation for quasi
one-dimensional disordered conductors in the unitary symmetry class is employed
to calculate all $m$-point correlation functions by a generalization of the
method of orthogonal polynomials. We obtain closed expressions for the first
two conductance moments which are valid for the whole range of length scales
from the metallic regime ($L\ll Nl$) to the insulating regime ($L\gg Nl$) and
for arbitrary channel number. In the limit $N\to\infty$ (with $L/(Nl)=const.$)
our expressions agree exactly with those of the non-linear $\sigma$-model
derived from microscopic Hamiltonians.
