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290                                                       P. LAZZERETTI ET AL.

                            6.  Fourth-order CHF energy


                             The CHF  formulae  (75)-(77) for  the  response tensors  are  established  by expanding
                             the Hartree-Fock energy  [8],




                             in powers  of the  electric  field in the  same way  as  (1). In  the  presence of  multiple
                             perturbations, the first-order perturbed  core Hamiltonian can  be  written



                             where the parameters a, b, c, etc., are related to the intensity of each perturbation.
                             The expansion for the energy of a molecule becomes









                             Comparing  this  general expression with  the  analogous expansion (1),  one  finds (no
                             sum over repeated  Latin  indices)
















                             It should be noted  that, in this notation, the order of the superscripts is irrelevant;
                                         is the  entire  perturbed  energy  term linear  in ab ... z and there  is no
                             additional term  with  permuted ab ... z indices.
                             The following  terms appear in the expression of the 4-th order energy
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