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186                                                      Y. G. SMEYERS ET AL.
                             In Table  5,  we  give the  HPHF  energy  values  obtained for  the  singlet  ground  state,
                             and the  first triplet and  singlet excited  states, as  well as  the RHF  and  UHF  values
                             obtained elsewhere [20]  with different basis sets.  It is seen that whereas  con-
                             formation is  the  preferred in  the  singlet  ground  state, the   one is  the most
                             stable in the excited states in accordance with the large band progressions observed
                             in the  electronic  spectrum, as  well as  the band  assignments  [20].  This  change of
                             conformational preference can be also interpreted on  the basis of the destabilization
                             of the   electronic system.
                             Here, once more the barrier height  values are seen to  be very  basis dependent. The
                             value encountered for  the singlet excited state,  however, is found  to be in  relatively
                             good  agreement  with the experimental  value:

                             3.4. FORMIC  ACID
                             Finally, the HPHF  approach  is  applied to the formic acid molecule, in  its first  singlet
                             excited state,  which is  not orthogonal  any  more to the  singlet ground  state  in a
                             random  conformation.
                             The calculations were performed into two basis sets,  with full geometry  optimization
                             except for  the  torsional  angles  and  Two  non  planar  conformations  were con-
                             sidered, which correspond to  minima on  the  potential  energy  surface into the GVB
                             approximation [21]. In these conformations, the molecule adopts a pyramidal confor-
                             mation, as in methanal.  In addition, the hydroxilic group  is rotated  up or down the
                             OCO plane.
                             In Table  6,  the  formation  energy  values for  these two  preferred  conformations are
                             given, together with the corresponding  values for the  planar conformations syn and
                             anti. It is seen that one of the minima is only slightly more stable than the other when
                             calucated with the larger basis, but much more stable than the planar  conformations
                             in accordance with the GVB  calculations  [21].



















                             The geometrical parameters found for these four conformations are gathered in Table
                             7. It  is  seen  that the  carbon  atom of the  preferred conformations  exhibits an
                             hybridization  because of  the  destabilization of  the  electronic  system by  the
                             antibonding  orbital,  whereas the  carbon atom  of  the planar  conformations  shows
                             mostly an    one.
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