Page 168 - Strategies and Applications in Quantum Chemistry From Molecular Astrophysics to Molecular Engineer
P. 168

QUANTUM CHEMISTRY COMPUTATIONS IN MOMENTUM SPACE                       153
                         converges to results close to HF limit, but obviously it cannot approach it completely
                         because the fit is based on a limited number of gaussian functions.


                         4. Results  and  advantages


                         In Tab.  1  are given the various results obtained in our group ; the precision of the method
                         used for the resolution as well as the main interest of these results are summarized. When
                         results have been obtained numerically (section 3.1) the method is denoted num-SCF or
                         num-MCSCF according to the level of theory used ; when an analytical treatment (section
                         3.2) has  been  performed, the  denotation is analyt-gauss if  the  trial functions  were
                         expressed as  linear  combinations of gaussian  functions or analyt-Slater if the  trial
                         functions  were  expressed as  linear combinations  of Slater  functions.  Finally  when a
                         semi-analytical treatment (section 3.3) has been done the method is called analyt-gauss*.
                         Results fall into three categories :  the first one corresponds to pure numerical results on
                                                  which have  demonstrated the  feasibility of  numerical
                         calculations.  They have also provided momentum wavefunctions for physical quantities
                         such as Compton profiles  [17],  (e,2e)  cross-sections  [26]. In  the  second category we
                         have investigated  the  possibilities of using a  variation-iteration  procedure  defined in
                         momentum  space to  improve the  one-electron  states for  various chemical systems
                         expressed as  linear combinations  of gaussian  functions. Significant  improvements in
                         energy quantities and properties  sensitive to the shape of the  wave  function  (Compton
                         profile, momentum distribution, etc.) were indeed noted. In particular, the first iteration
                         transforms the trial  wave function expressed as  linear combinations of gaussian functions
                         in an expression which involves Dawson  functions. An asymptotic analysis carried on
                         the first iterate discloses a behavior quite close to the exact one. In the third category, the
                         semi-numerical approach is used to provide physical quantities.  Similarly to the position
                         space approach it  is based on  the  variation principle  which  guides the changes  of the
                         wavefunction :  the  closer the  energy E  to   the  nearer the  trial  wave function  the
                         ground  state  In  LCAO-SCF-MO schemes  however, the  function  obtained by
                         minimizing the total energy does not necessarily give a good description of properties
                         such as multipole moments, while in momentum space due to the capacity of the method
                         to improve the quality of a wavefunction significant improvements have been obtained
                         e.g. for the dipole moment of the hydrogen fluoride [38].
   163   164   165   166   167   168   169   170   171   172   173