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Convergence of Expansions in a Gaussian Basis




                        W. KUTZELNIGG
                        Lehrstuhl für Theoretische Chemie, Ruhr- Universität Bochum,
                        Universitätsstr. 150,  D-4630 Bochum,  Germany



                        1. Introduction
                        Few papers have had as much impact on the progress of ab-initio quantum chemistry
                        as that of Boys [1]  where he proposed to use Gaussians  (GTOs) as basis sets.  The
                        great breakthrough of ab-initio theory would never have been possible without the
                        invention of  Gaussians.  Nevertheless,  even  nowadays it is  difficult to  explain to
                        a beginner why one  should rely  on  Gaussians,  which  have the  wrong behaviour
                        both  near the  nuclei and very far  from  them. The  ease;  with  which  two-electron
                        integrals over  GTOs can be computed is certainly an argument.  However, if one
                        has thought  a  little  bit on the  importance of  choosing basis sets  with the  right
                        behaviour at  the  singularities of  the  Hamiltonian  [2],  one  cannot but be  deeply
                        surprised  that  expansions in  GTOs converge decently  well in  spite of their  failure
                        at the singularities of the Hamiltonian.
                        To appreciate  this point  somewhat  better it  is  useful to  compare  three  types of
                        Gaussian basis sets, (a)  a set of Gaussians with common orbital exponents (for one
                        l)  but a sequence of principle quantum-numbers




                        (We consider here only the case of a single center), (b)  the same set (1.1) but with
                        n – l = 1,2,3,4, ..., (c) a set of Gaussians with the lowest possible n for each l, but
                        with a sequence of orbital exponents




                        Sets of orbital  exponents   have  been proposed mainly by Huzinaga  [3], van
                        Duijneveldt [4], Pople et al.  [5]. A systematic construction of basis sets of arbitrary
                        dimension is  possible in  terms of the  ’even tempered’  concept of  Ruedenberg et
                        al. [6,7  ],  or  of  some  more sophisticated generalizations  [8,9,10]. For  a  recent
                        comprehensive review on basis sets see Feller and Davidson [11].

                        It does not  make a significant difference that in practice one uses  ’cartesian Gaus-
                        sians’  rather  than  Gaussians with  explicit inclusion  of spherical  harmonics. One
                                                            79
                        Y. Ellinger and M. Defranceschi (eds.), Strategies and Applications in Quantum Chemistry, 79–101.
                        © 1996 Kluwer Academic Publishers. Printed in the Netherlands.
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