1999
DOI: 10.1007/3-540-48972-x_4
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An Introduction to the Theory of Geminals

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Cited by 147 publications
(91 citation statements)
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“…1 They are based on the ansatz of antisymmetrized product of twoelectron functions called geminals. The resulting optimization problem is, in general, involved unless geminals are restricted to be strongly orthogonal that leads to the antisymmetrized product of strongly orthogonal geminal (APSG) theory.…”
Section: Introductionmentioning
confidence: 99%
“…1 They are based on the ansatz of antisymmetrized product of twoelectron functions called geminals. The resulting optimization problem is, in general, involved unless geminals are restricted to be strongly orthogonal that leads to the antisymmetrized product of strongly orthogonal geminal (APSG) theory.…”
Section: Introductionmentioning
confidence: 99%
“…1 The simplest variant of such a model represents wavefunctions as a single antisymmetrized product of strongly orthogonal geminals ͑APSG͒. [2][3][4][5][6][7] Sometimes this model is referred to as separated electron pair ͑SEP͒ theory. [8][9][10][11][12] Most prior studies focused on the total amount of correlation energy recovered by the product of strongly orthogonal geminals.…”
Section: Introductionmentioning
confidence: 99%
“…The third order CMX correction, however, is not zero, and it often represents a considerable improvement. This is illustrated on the example of the symmetric dissociation curve of the water molecule in 6-31G basis set, where the CMX correction is shown as applied to the Hartree-Fock (HF) and the antisymmetrized product of strongly orthogonal geminal [164] (APSG) approximations.…”
Section: Optimized Unsøld Approximation: Cmx2mentioning
confidence: 99%
“…The pioneering work in this direction by Dyall [155] was followed in Malrieu's [76,156] and Mukherjee's [157,158] laboratories. In our group, we have developed [159][160][161][162][163] a specific PT to perturb the antisymmetrized product of strongly orthogonal geminal [164] (APSG) wave function, where the geminals are eigenfunctions of an effective two-body Hamiltonian. Inclusion of explicit two-body terms is conceptually an appealing feature, but complicates the formalism significantly.…”
mentioning
confidence: 99%