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FSGO Hartree-Fock Instabilities of Hydrogen in External Electric Fields




                        J.M. ANDRE,  G. HARDY, D. H. MOSLEY and L. PIELA
                        Facultés Universitaires Notre-Dame de la Paix, Laboratoire de Chimie Théorique
                        Appliquée,  61 rue de Bruxelles, B-5000 Namur, Belgium and University of Warsaw,
                        Quantum Chemistry Laboratory, Pasteura 1, 02-093 Warsaw, Poland



                        1. Introduction

                        In the early  sixties, it was  shown by Roothaan  [1]  and  Löwdin  [2]  that the symmetry
                        adapted solution  of the  Hartree-Fock  equations  (i.e.  belonging to  an irreducible
                        representation of  the  symmetry  group of  the Hamiltonian) corresponds to  a  specific
                        extreme value of the total energy. A basic fact is to know whether this value is associated
                        with the  global  minimum or a  local  minimum,  maximum or even  a  saddle  point of the
                        energy. Thus, in principle, there may be some symmetry breaking solutions whose energy
                        is lower than that of a symmetry adapted  solution.

                        The Hartree-Fock description of the hydrogen molecule requires two spinorbitals, which
                        are used  to  build the  single-determinant  two-electron  wave function. In  the Restricted
                        Hartree-Fock  method  (RHF)  these two  spinorbitals are  created from  the same  spatial
                        function  (orbital) but differ only by  its multiplication by the a  or  spin basis functions.

                        It is common knowledge that, in the case of the hydrogen molecule studied in a minimal
                        basis set, the correlation error can be explained by  the existence of ionic  species in the
                        hydrogen dissociation products:




                        This is  an  artefact due  to  the  non-zero  probability of the  restricted  wave-function of
                        finding two electrons of opposite spins at the same spatial position.
                        FSGO's (Floating Spherical Gaussian Orbital) were introduced by  Frost [3]  in the mid
                        1960s.  With  FSGO's one  abandons the idea  of  atomic  orbitals  centred on  nuclear
                        positions to  arrive at  an even more  compact basis set  than  a  minimal one.  FSGO's
                        correspond to  s-type  Gaussians that are  not fixed at  the  atomic  centers but  are able to
                        "float" in space so as to optimally represent each localized pair of electrons.  Because only
                        one function  is needed for each  electron  pair, the  basis set  used  is often referred to as
                        being "subminimal".
                                                           189
                        Y. Ellinger and M. Defranceschi (eds.), Strategies and Applications in Quantum Chemistry, 189–202.
                        © 1996 Kluwer Academic Publishers. Printed in the Netherlands.
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