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264                                             M. TADJEDDINE AND J. P. FLAMENT
                              For a  heteronuclear diatomique  molecule of   symmetry (z being  the molecular
                              axis), it becomes :


                              with :








                             where    is  the electron number. As   tends to  zero, the constants  tend  to





                              The normalization condition         imposes to move the origin to the center of
                              electronic charge                 thus, the  polarizability may be  written very
                              simply in the limit of zero frequency :







                              2.1.3. A  mixed  approach

                              The idea to combine a  method only  polynomial  (Eq.6 with  and     )  with
                              the SCF–CI  procedure (Eq.5 with            )  has  been initially developed for
                              the calculation of magnetic observables (9) and later for the electric ones (10). Thus,
                              the first–order perturbed wavefunction is given by  :





                              and the component    of the polarizability tensor becomes :





                              The calculations  of the   and   constants  lead to  a system  of linear equations
                              similar to that of the SCF–CI method, but with three more lines and columns corre-
                              sponding to the coupling of the polynomial function  with the electric field  perturba-
                              tion. The methodology and  computational details have already  been discussed (1);
                              we stress two points :  the role of the dipolar factor, the  nature and  the number of
                              the excited states to include in the summation.
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