Geometrical effects on the pairing process between electrons and betwe
en holes are comparatively studied by using an attractive Hubbard Hami
ltonian. For triangular lattices, it is found that the hole pairing is
always stronger than the electron case due to the frustration of anti
-bonding states; contrary to that occurred in bipartite lattices, wher
e there is a complete symmetry between the electron and hole pairings.
The ground state of two holes, when the attractive nearest-neighbor i
nteraction is dominant, is surprisingly triplet and its wave function
has directional nodes. On the other hand, the hole pairing in disorder
ed lattices is analyzed and the results show an enhancement of the pai
r-binding energy as the self-energy difference increases in a random b
inary alloy A(x)B(1-x). This fact suggests that the pairing process is
highly sensitive to the one-particle localization condition. The grou
nd-state phase diagram for the case of on-site interaction disorder sh
ows regions where pairing is avoid for ordered diatomic systems but no
t for disordered cases.