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Ab–initio Calculations of Polarizabilities in Molecules:  Some Proposals to
                        this Challenging Problem


                        M. TADJEDDINE, J.P.  FLAMENT
                        Ecole  polytechnique,  D.C.M.R., 91128  Palaiseau Cedex,  France




                        1.Introduction

                        The polarizability expresses the capacity of a system to be deformed under the action
                        of electric  field :  it is  the  first–order  response. The  hyperpolarizabilities  govern the
                        non linear processes which appear with the strong fields. These properties of materials
                        perturb the propagation of the light crossing them; thus some new phenomenons (like
                        second  harmonic and  sum  frequency  generation) appear,  which  present a  growing
                        interest in  instrumentation with the  lasers development. The necessity of prediction
                        of these observables requires our attention.
                        The calculation  of the static polarizability,   is now well documented, actually com-
                        mon enough  to give a test  for the  choice of the  atomic basis sets  in  molecular cal-
                        culations. On  the other hand, few calculations concern the dynamic polarizability,
                        i.e. when  the   energy of the electric field is no more zero but  can  vary and  reach
                        the electronic transition  energies of the molecule.  Computations are  more complex;
                        not only  they  must  well  describe the  ground state in order  to  reproduce the  static
                        polarizability, but  also the excited states  (valence and  Rydberg  states)  in order to
                        give the resonance energies correctly.
                        The computation of these observables poses several problems :

                           •  In the case of an electromagnetic perturbation, a first difficulty rises :  the choice
                             of the  gauge.  Indeed  the gauge   is  only a  mathematical  tool and  the
                             observables of  interest  (energies,  susceptibilities...) must  be  gauge invariant;
                             they  are effectively if  the computations  use complete molecular  bases. Our
                             calculations,  using  bases  unavoidably truncated,  will be never gauge  invariant.
                             The discrepancies with respect to the gauge invariance is, in a way, a mesure of
                             the quality of our computation, of the molecular basis  set. In our  calculations
                             the gauge     is used.

                           • Since we must restrict the number,N, of the molecular states used in the com-
                             putations, what  value have we  to give to N ?  And then, can  we  correct the
                             obtained value for the polarizability in order to approximate to the exact value
                             by evaluating the ignored terms ?
                           • The formula which gives the polarizability involves the excited states.  As  said
                             before, it is necessary to be able to well describe them. The choice of the atomic
                                                           261
                        Y.  Ellinger and M. Defranceschi (eds.), Strategies and Applications in Quantum Chemistry, 261–278.
                       © 1996 Kluwer Academic Publishers. Printed in the Netherlands.
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