Numerical results pertaining to the distribution of the conductance peak sp
acings of disordered interacting quantum dots are presented. The ground sta
te of a dot was calculated by an exact diagonalization of a tight-binding H
amiltonian for different values of interaction strength, lattice sizes, num
ber of electrons and disorder. It was found that the distribution depends o
n the interaction strength. For a large range of interactions which corresp
ond to a regime in which the correlation between the electrons in the dot e
xhibit intermediate-range order, the distribution is Gaussian with a width
proportional to the charging energy. This behaviour is different from the d
istribution in the weak-interaction limit which is well described by a cons
tant-charging random matrix theory. Recent experiments measuring the additi
on spectrum of quantum dots are performed at densities corresponding to the
intermediate-range order regime and exhibit Gaussian distributions of the
spacings.