Page 75 - Strategies and Applications in Quantum Chemistry From Molecular Astrophysics to Molecular Engineer
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60                                                            C. VALDEMORO
                            the element of   (relation 16), which appears between brackets, by its value in terms
                            of the electronic integrals  (relation 8) one gets after some simple algebra






                            At first  sight,  this looks  rather complicated, and  in fact, evaluating this general rela-
                            tion is not trivial. On the other hand, the results are simple, closed form expressions.
                            The derivation of the algorithms for different values of p have been described in detail
                            previously [25,26,28]. Here we will just sketch the results obtained.
                            The main point  about  the SRH matrix is that its only non  zero elements are those
                            where the set of the i  indices and  the set of the j indices  are equal or  differ at  the
                            most in two indices.
                            The general form of the three different classes of the matrix elements are  [28]:

                               • The set of i indices is equal to the set of j indices (although any ordering of the
                                 indices is allowed).





                                 Where the symbol    has  the same meaning as previously.  In this relation,
                                 denotes a permutation of the indices     and A and B are coefficients.
                               • An  index  of  the  set i differs from  that of an index  of  the set j, say
                                 (although any ordering of the indices is allowed).





                               •  Two indices  of  the set i differ  from two indices  of  the set j, say   and
                                        (although any ordering of the indices is allowed).




                            A very  convenient  feature of this formalism  is  that the  values of the A and B coef-
                            ficients only depend on three numbers: the number of electrons (N), the number of
                            orbitals of the basis (K), and the Spin quantum number (S).
                            The different  orderings of  the  matrix  element indices (   superscript in relations
                            19,20,21) give rise to different values of the A and B coefficients.  Finally, the value of
                            these coefficients also depends on whether one or more of the matrix element indices
                            are repeated  (appears  twice).
                            For p = 1,2,3  the  values  of these  coefficients have been  explicitly obtained;  and  for
                            large p, a set  of diagramatic rules have been reported  [28] in order to determine the
                            coefficients in each case.
                            To calculate a p – SRH once the electronic integrals are known, is therefore a very
                            simple and  rapid task.
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