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A COUPLED MCSCF-PERTURBATION TREATMENT OF ELECTRONIC SPECTRA            51

                         The comparison  to the  results  obtained  using the  SCI/MP2 approach [45,68]  leads to
                         unquestionable conclusions: not  only  the  SCI/MP2  method  does not  provide acceptable
                         transition energies for the lowest valence and Rydberg states but it misses some of them
                         and does  not provide any good energetical ordering of the excited states.  Even if this
                         method presents interesting computational advantages, it can only provide a flimsy
                         quantitative electronic spectrum, as anticipated in section 3.1 and outlined in reference [22].


                         5. Conclusions  and prospects
                         The present approach  is one of the  second-generation  multireference perturbation treatments
                         first opened by the CIPSI algorithm 20 years ago. Even if the spirit of these new treatments
                         is different, mainly because the reference space is chosen on its completeness rather than on
                         energetical criteria, it remains that the unavoidable problems of disk storage, bottleneck of
                         variational approaches, can now be conveniently transferred to the problem of CPU time
                         which is less restrictive.
                         The methodology presented here expands the recent CASPT2 approach to more flexible
                         zeroth-order variational spaces for a multireference perturbation,  either in  the Moller-Plesset
                         scheme or in Epsein-Nesbet approach [70-72]. Furthermore, it allows for the use of a wide
                         set of possible correlated orbitals.  These two last points were  discussed elsewhere  [34].
                         The reliability of this method for the evaluation of (vertical) electronic spectra has been
                         clearly  established in  the  present  work, and  further calculations on  other molecules
                         (ethylene, vinylydene… for example) have confirmed the very promising potentialities of
                         such an approach that avoids the possible artefacts brought in by any arbitrary truncated
                         CIs when dealing with excited states  [49]. We also emphasize that this methodology is able
                         to give reliable splittings between states ranging from  10 kcal/mol to more than 10 eV.


                         References

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