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106                                             J. P. MALRIEU AND J. P. DAUDEY
                             t  being the hopping  integral  and          the on-site  effective  bielectronic
                             repulsion, while the radius of convergence of the Rayleigh Schrodinger perturbation theory
                             from the RHF single determinant is



                             For      the relevant perturbation consists in perturbing the covalent (or neutral) VB
                             structures by their interaction with the ionic ones; this is the strongly correlated or magnetic
                             domain. So that the Hartree Fock symmetry breaking occurs in a zone which covers the
                             whole magnetic domain and a significant part of the "weakly" correlated domain


                             2.3.     THE  MULTIPLE BOND

                             For more complex problems such as multiple bonds                and  Metal-
                             Metal bonds  [15-17]) or extended systems ( the   system of cyclic polyenes,  among
                             others), the symmetry-breakings may take several forms since one may leave different
                             space-and  spin-symmetry  constraints independently  or simultaneously.  For   for
                             instance, the RHF symmetry adapted solution is of   character        while
                             one may find at much  lower energy a   solution  of  closed shell character (a  pure
                             singlet) which has broken the symmetry between the x and   bonds. A UHF solution lies
                             much below, which has a dominant VB character

                             at short interatomic distances and a correct asymptotic  content




                             at large interatomic distances.
                             The multiplicity of symmetry breakings  have been explored in details in  where they
                             occur near the equilibrium interatomic distance [12].
                             The fact that symmetry breaking occurs at shorter interatomic distances for multiple bonds
                             than for single bonds may be understood within two different languages. One refers to the
                             instability conditions of the symmetry-adapted solution. In multiple bonds some bonding
                             electron pair are strongly delocalized and would not break the symmetry (for instance the
                                       while the p bonds are weaker and enter more rapidly into the :



                             regime (this criterion  is only weakly modified for multiple bonds [12]  ). Of course in a
                             sextuple  bond, as   the   bonds are so  weak  that they  induce a  strong symmetry
                             breaking  [18].
                             In the other approach one looks at the VB content of the symmetry adapted) wave function,
                             for instance for
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