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AB INITIO CALCULATIONS OF POLARIZABILITIES IN MOLECULES               269
                        where    and   are  the well known  Dunham constants and   and   the values
                        of the first  and second derivatives of the polarizability calculated at  the  equilibrium
                        geometry.
                        By including the effect of the rotation  (at  a given T temperature, for the level v = 0)
                        in a perturbation calculation, we have obtained (5)  :





                        where we have introduced the dimensionless constant c like :




                        which characterizes the molecule (m is its reduced mass).
                        Moreover, for  the observables  depending on  external  electric field, its  specific  effect
                        has to be investigated :  the electric field induces new terms in the nuclear Hamilto-
                        nian, due to the change of equilibrium geometry and the nuclear motion perturbation.
                        Pandey and Santry (14) has brought to the fore this effect and calculated the correc-
                        tion which only concerns the parallel component.  It is represented by the following
                        expression :



                       where    is  the  value of the first  derivative of the dipole moment calculated at  the
                        equilibrium  geometry. On table 2  we  have reported the  results  obtained for  the




















                        static polarizability of CO : the correction for the perpendicular component may be
                        neglected; for the parallel component, the vibronic correction mainly originates  from
                        the effect of the electric field cannot  be neglected at  all.

                        2.6.  RESULTS FOR THE POLARIZABILITY OF  CO
                        The quality of electronic calculations is confirmed by the very good  agreement of the
                        resonance energies for both  components if we compared to the experimental ones,
                        as shown on table 3.
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