We study the difference between on site Hubbard and long range Coulomb repu
lsions for two interacting particles in a disordered chain. The system size
L tin units of the lattice spacing) is of the order of the one particle lo
calization length and the energies are taken near the band center. In the t
wo cases, the limits of weak and strong interactions are characterized by u
ncorrelated energy levels and are separated by a crossover regime where the
states are more extended and the spectra more rigid. U denoting the intera
ction strength and t the kinetic energy scale, the crossovers take place fo
r interaction energy to kinetic energy ratios U/t and U/(2tL) of order one,
for Hubbard and Coulomb repulsions respectively. While Hubbard repulsion c
an only yield weak critical chaos with intermediate spectral statistics, Co
ulomb repulsion can drive the two particle system to quantum chaos with Wig
ner-Dyson spectral statistics. The interaction matrix elements are studied
to explain this difference.