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HARTREE-FOCK MODEL TO THE LOWEST SINGLET AND TRIPLET EXCITED STATES    187














                        Distances in   and  angles in degrees.



                        4. Discussions and conclusions
                        In the present paper, the Half-Projected model is applied to the direct determination
                        of the lowest singlet and triplet excited states in which  just as the usual UHF
                        method is  employed for  states in which           As  examples, the method
                        is successfully applied to  the calculation of some molecular properties of methylene,
                        methanal, dimethylglyoxal and formic acid, in these excited states.
                        In  the case of methylene,  methanal or  dimethylglyoxal, in  which the excited wave-
                        function is  always orthogonal  by symmetry  to  that of the  singlet  ground  state, the
                        procedure converges well without any complication. In this case, the HPHF method
                        could be  regarded as  an  extension of  the  usual UHF  procedure  for the  states in
                        which           This extension  appears to  be  especially interesting for  the  direct
                        determination of the lowest singlet excited states of medium size molecules, for which
                        no simple and efficient method exists.
                        In the case of formic acid, in a random conformation, the excited wave-function pos-
                        sesses the  same  symmetry  as  that  of the ground state.  In  the  present paper, we
                        propose to  orthogonalize the excited  orbital to  its  companion in  order to  avoid the
                        variational  collapsing of the excited state  into the fundamental one.  The procedure
                        converges more slowly, but  procedures for  accelerating convergence may be used.  No-
                        tice that the excited wave-function is not  necessarily orthogonal to the fundamental
                        one in this way of proceeding. But, both functions have not to be orthogonal because
                        the Hamiltonian operators (24) and (37) are not the same. They may expected, how-
                        ever, to be nearly orthogonal.  It may be added here that a complete orthogonalization
                        will yield probably worst results [15].
                        It may be concluded thus that the Half-Projected Hartree-Fock model proposed  more
                        than two  decades ago  for  introducing some  correlation  effects in  the  ground  state
                        wave-function [1,2],  could be  employed  advantageously for the  direct determination
                        of the  lowest  triplet and  singlet excited  states, in which  This  procedure
                        could be especially  suitable for  the  singlet excited  states of medium size  molecules
                        for which no other efficient procedure exists.

                        References
                          1. Y.G.  Smeyers, An.  Fis.  (Madrid), 67,  12  (1971).
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