We study the superconducting instabilities generated by the inclusion
in the Anderson lattice model of a density-density attractive potentia
l between correlated electrons on nearest-neighbouring sites. Using a
description of the normal phase based on a perturbative expansion arou
nd the atomic limit, we treat the attractive potential in the broken-s
ymmetry Hartree-Fock scheme and analyze which of the possible symmetri
es of the superconducting order parameter leads to the highest possibl
e transition temperature in the case of a two-dimensional square latti
ce. For values of the on-site f-repulsion large compared to the hoppin
g amplitude, a suppression of any possible superconducting phase occur
s, regardless of the symmetry of the order parameter.