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46                                                 O. PARISEL AND Y. ELLINGER












































                             We emphasize that the Rydberg states are included in the variational MCSCF treatment in
                             order not to be undercorrelated relative to the valence states [48,49]. Furthermore, it is seen
                             that all  the previous distributions are coupled to diexcitations  from the   to the
                             orbital: that way, we account for the non-dynamical repolarization of the polar  bond  in
                             a GVB-like approach.
                             Finally, we  also  account for an  explicit relaxation of both lone pairs  of   by  the
                             inclusion of corresponding correlating orbitals [50] and treat them at a GVB-like level.
                             The final space spanned by these distributions can then roughly be seen as a product of
                             CAS, GVB and MCSCF spaces. It accounts for all effects supposed to be essential to get a
                             good zeroth-order  description of  the  ground and the  excited valence and  Rydberg
                             states.The dynamical correlation of the 8 electrons  included in this variational treatment
                             will be recovered, in the ground state and in the excited states, with the perturbation, and so
                             will be the correlation energy arising from the core and from the   remaining  electrons.
                             The perturbation will also  account for  any  coupling not  explicitely included  in  the
                             distributions presented in Table 1.
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