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QUANTUM CHEMISTRY COMPUTATIONS IN MOMENTUM SPACE                       151

                        Fourier transform of orbital products :






                        Electronic repulsion term :














                        Exchange term :














                        So the first iteration transforms the trial  wave functions expressed as linear combinations
                        of gaussian functions into an expression which  involves Dawson functions  [62,63]. We
                        have not been able to find a tabular entry to perform explicitly the normalization of the first
                        iterate, accordingly this is carried out numerically by the Gauss-Legendre method [64].

                        One of  the drawbacks  of  the  first  iteration,  however, is  that computation of  energy
                        quantities, e.g. orbital and total energies, requires to evaluate the integrals occurring in
                        Eq.  3 on the basis of the   Unfortunately, the transcendental functions in terms of
                        which the      are expressed at the end of the first iteration do not lead to closed form
                        expressions for these  integrals and a  numerical  procedure is  therefore  needed.  This
                        constitutes a barrier to carry out further iterations to improve the orbitals by approaching
                        the HF limit.  A compromise has been proposed between a fully numerical scheme and the
                        simple  first iteration  approach  based on  the  fact that at the end of each  iteration the
                                 entail the  main  qualitative  characteristics of  the  exact  solution and  most
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