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AB INITIO CALCULATIONS OF POLARIZABILITIES IN MOLECULES                267
                            where    and     are  the polarizabilities calculated with N states, with and
                            without the ”polynomial”  contribution. The value of the exponent p is  deter-
                            mined by a least– square fit and then the extrapolated polarizability is obtained
                            by a linear regression.  In the case of the dynamic polarizability, this extrapo-
                            lation is done separately for the  cases  and
                       Figure (1) gives an illustration of this extrapolation procedure for the calculation of
                       the static parallel polarizability in CO. In this case the extrapolated value
                       was obtained with the following equation

                       It is important to underline two points  :

                          • The extrapolation procedure rests upon the hypothesis of exact or very accurate
                            eigenstates   which in practical calculations is seldom the case for the large
                            molecules. The function    partly  compensates the  weakness of the  atomic
                            and molecular basis sets with the extrapolation  procedure.
                          •  This extrapolation has  been obtained with  a  finite  number N (usually  less
                            than 10) of spectral states lying under the first ionization potential;  thus, the
                            continuum is not taken into account explicitly in our calculations.  It has been
                            simulated through the   function and the extrapolation procedure as we are
                            going to show it.

                       2.4. CONTINUUM CONTRIBUTION

























                       Hydrogen atom, in its ground state, can be treated in an entirely analytic approach.
                       The calculation of the second–order perturbed energy gives the well known values :

                       for the static polarizability of the ground  state.  Since we have used exact  analytic
                       wavefunctions which are the eigenstates of the electronic Hamiltonian, the continuum
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