We apply the Hubbard Hamiltonian to describe quantum-dot arrays weakly
coupled to two contacts. Exact diagonalization is used to calculate t
he eigenstates of the arrays containing up to six dots and the linear-
response conductance is then calculated as a function of the Fermi ene
rgy. In the atomic limit the conductance peaks form two distinct group
s separated by the intradot Coulomb repulsion, while in the band limit
the peaks occur in pairs. The crossover is studied. A finite interdot
repulsion is found to cause interesting rearrangements in the conduct
ance spectrum.