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MOLECULAR ORBITAL ELECTRONEGATIVITY AS ELECTRON CHEMICAL POTENTIAL     125

                        in an iterative MO-LCAO scheme using as an AO basis maximum localization hybrids
                         [12],  Hoffman’s  atomic parameters  [13], and  Cusachs’ expression  [14] for  the  off-
                        diagonal elements  of  the  Hamiltonian  .  Since  this is  just an illustration  of  the
                        numerical aspects of the equations given above, we need not justify further the scheme
                        used. The special features which  make the  present example especially  suited for our
                        purpose  include the fact  that in the case of the  system the MO occupation numbers
                        must be  given the  values 2,  1.5, 0  (in  the  order of increasing  orbital  energies) in
                        order to ensure the equivalence between the two  degenerate   systems of our linear
                        molecule. This  feature is  especially important  since   of eqn 28 is the  sum  of
                        terms containing as factors the differences between MO occupation numbers
                        This fact  implies that  only  MO's with  different  occupation  numbers play  a role in
                        the terms  by  which eqn  38 differs  from the  simpler  form 39.


                               Table 1:  Source  data and     for the  average  system  of  FeCO
                        a. Overlap matrix for one   system of FeCO

                                                   1.0000  0.2783     0
                                                   0.2783  1.0000  0.2414
                                                        0 0.2414  1.0000

                        b. Ham.  matrix (eV) with  correction at convergence
                                                  -9.6177  -2.2081      0
                                                  -2.2081 -10.9490  -2.7811
                                                      0   -2.7811  -12.6638
                        c. Eigenvalues (italics, eV) and Löwdin charge bond-order matrix

                                                 -12.7349 -11.4723  -9.4836
                                                   0.7671   0.5442 -0.0530
                                                   0.5442  -0.2747  0.0418
                                                  -0.0530   0.0418  -0.4924

                        d. Derivative of P with respect to   and diagonal  elements of   (italics)
                                                   0.2087  -0.4060  -0.0689
                                                  -0.4060  0.7583 0.1859
                                                  -0.0689   0.1859  -0.0281
                                                   0.1502  0.8355  0.0142



                        The source matrices (for the sequence Fe C  0)  are presented in Table 1  together with
                        the resulting  derivative of the  Löwdin  population  matrix P. The  electronegativities
                        derived from the complete expression 38  and from the approximate expression 39  are
                        -7.1690 eV and -7.3582 eV, respectively, thus suggesting that even in the unfavourable
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