1992
DOI: 10.1002/qua.560420416
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On the evaluation of overlap integrals with exponential‐type basis functions

Abstract: The numerical properties of a one-dimensional integral representation [H. P. Trivedi

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Cited by 49 publications
(14 citation statements)
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“…Then we obtain where n ³ l, n¢ ³ l¢+1, l¢ ³ 1, t = 0 and the coecients a l and b l are determined by following equations: The values of the Gaunt coecients and the Gegenbauer coecients should be known to calculate the radial part of overlap integrals with the same screening parameters, by using Eq. (9). Gegenbauer coecients were calculated from Eq.…”
Section: The Expression For a S Nlk;n H L H K In Terms Of Auxiliary Fmentioning
confidence: 99%
See 1 more Smart Citation
“…Then we obtain where n ³ l, n¢ ³ l¢+1, l¢ ³ 1, t = 0 and the coecients a l and b l are determined by following equations: The values of the Gaunt coecients and the Gegenbauer coecients should be known to calculate the radial part of overlap integrals with the same screening parameters, by using Eq. (9). Gegenbauer coecients were calculated from Eq.…”
Section: The Expression For a S Nlk;n H L H K In Terms Of Auxiliary Fmentioning
confidence: 99%
“…Some kind of ETOs, called B functions, in which radial parts are reduced to Bessel functions have been studied in Refs. [7,8,9,10,11,12,13] for the evaluation of overlap integrals.…”
Section: Introductionmentioning
confidence: 99%
“…An alternative approach which we propose here relies on the recursive relations (4) and (5). By inserting them into the definition (30) one arrives at…”
Section: A Spin-averaged Potentials Iaaa Typementioning
confidence: 99%
“…Nonetheless, a considerable interest has remained in the field of Slater-type orbitals (STOs) [3,4] or more general exponential-type orbitals (ETOs) [5,6]. This is motivated mainly by the superior analytical properties of STOs (i.e., fulfilment of the nuclear cusp condition [7] and correct long-range decay [8,9]) and their formal simplicity.…”
Section: Introductionmentioning
confidence: 99%
“…Since the enrichment functions are sharp and localized, we resorted to high-order tensor-product quadrature to obtain the results shown in Figure 6 [61]; however, for the method to be viable, efficiency in computing the stiffness matrix and force vector entries (Kd = f ) is paramount. For the integration of functions with peaks at or near a boundary over the interval, the Möbius transformation has been adopted in quantum chemistry [93][94][95]; for electronic-structure calculation with a 1/r term in the integrand of the Hamiltonian, Batcho [46] used the Duffy transformation [96,97]. In general, since the atom can be located anywhere inside the element, the above approaches do not meet our needs.…”
Section: Adaptive Quadraturementioning
confidence: 99%