“…The inclusion of the scale factor (R 1 R 2 R 3 ) 1/2 in order to get the standard normalization of the total wave function ⌿(R 1 ,R 2 ,R 3 ) leads to the final Hamiltonian expression which we have given in detail elsewhere for the case of zero total angular momentum. 17 As in our previous work, we have expanded the wave function in terms of a set of distributed Gaussian functions 28 ͑DGF's͒ which take into account the proper symmetry of the system. 16,17 After careful numerical tests, we have finally employed a basis of 22 Gaussian functions which depend on each atom-atom pair coordinate and are centered as follows: 3,3.7,...,12.1,13,14,...,17,20,23, and 26 Å.…”