2000
DOI: 10.1002/1097-461x(2001)81:1<16::aid-qua5>3.0.co;2-a
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Four-center integrals for Gaussian and exponential functions

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Cited by 41 publications
(17 citation statements)
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“…(5) and (6) are expressed in terms of overlap integrals so that we limit our comments to these latter. We developed algorithms for these in the context of the Gauss transform,17 one‐center two‐range expansions16, 18 (Barnett and Coulson's α function method19) a one‐center one‐range expansion technique of our own20, 21 and, recently, with the shift‐operators technique 10, 22. All these algorithms allow us a very efficient calculation of the overlap integrals, and no important differences in their performance are found.…”
Section: Algorithms For Integrals: Efficiencymentioning
confidence: 99%
“…(5) and (6) are expressed in terms of overlap integrals so that we limit our comments to these latter. We developed algorithms for these in the context of the Gauss transform,17 one‐center two‐range expansions16, 18 (Barnett and Coulson's α function method19) a one‐center one‐range expansion technique of our own20, 21 and, recently, with the shift‐operators technique 10, 22. All these algorithms allow us a very efficient calculation of the overlap integrals, and no important differences in their performance are found.…”
Section: Algorithms For Integrals: Efficiencymentioning
confidence: 99%
“…These include the Coulomb Sturmians introduced by Shull and Löwdin [46] and used by some other authors [47][48][49][50]. The shift operator technique [51][52][53] is a very elegant method which generates integrals with arbitrary STOs starting with the simplest integrals with 1s functions by application of the so-called shift operator. Gill et al [54,55] introduced the Coulomb resolution techniques where the interaction potential is expanded in terms of the so-called potential functions resulting from the the Poisson equation.…”
Section: Introductionmentioning
confidence: 99%
“…In quantum chemistry research, the mathematical description of atomic orbitals have been studied mainly with the use of Slater [25, 26] and Gaussian functions [27–29]. The Slater function has the correct cusp at the origin and the physical exponential decay at long range [30, 31], expected by the orbital representation, nevertheless, when a many‐electron system is taken into account, the matrix elements become very hard to calculate in the coordinate space [32].…”
Section: Introductionmentioning
confidence: 99%