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146                                                 M. DEFRANCESCHI ET AL.
                              Nuclear attraction, electron-electron repulsion and exchange terms.  Using the Eqs. 6 and
                              7, these contributions are respectively written in terms of the quantity Wij(q) previously
                              defined in Eq. 11 :












                              and






                              The detailed expression for  is then :












                              The momentum space equivalent of the total energy E, is :












                              3. Principles  for numerical  resolutions

                              Because of the terms    and      explicit  solutions to Eq. 3 cannot be obtained in
                              position space. In such cases approximate solutions are usually expressed as truncated
                              linear combinations of basis functions (LCAO expressions). In spite of its successes, the
                              LCAO approximation  experiences various  difficulties  (truncation limits,  nature of the
                              basis  functions,  etc.) hard  to  estimate and  which are  not entirely  controllable [51].
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