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Approximations to Self-Consistent Field Molecular Wavefunctions
Author(s) -
Thomas A. Halgren,
William N. Lipscomb
Publication year - 1972
Publication title -
proceedings of the national academy of sciences
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 5.011
H-Index - 771
eISSN - 1091-6490
pISSN - 0027-8424
DOI - 10.1073/pnas.69.3.652
Subject(s) - wave function , physics , electron , field (mathematics) , basis set , slater integrals , coulomb , matrix (chemical analysis) , atomic orbital , slater determinant , atomic physics , quantum mechanics , molecule , chemistry , mathematics , chromatography , pure mathematics
Unparameterized and parameterized versions are outlined of a new method for approximating self-consistent field wavefunctions from first principles at the minimum basis set level for complex molecules containing hydrogen and first-row atoms. The Hartree-Fock self-consistent field equations for closed-shell molecules are solved, retaining all one-electron integrals, and approximating the two-electron Coulomb integrals, hybrid integrals, and exchange integrals of the form (i(A)j(A)[unk]i(A)j(A)) and (i(A)j(B)[unk]i(A)j(B)) for centers A and B. A symmetrically orthogonalized basis set is used and rotational invariance is achieved by transformation to local axes that are unique for atoms in anisotropic environments. Parameterization based upon first-principle self-consistent field wavefunctions for a large number of molecules yields F-matrix elements to 0.007 atomic units (au), density matrix elements to 0.007 electrons, orbital populations and atomic charges to 0.01-0.02 electrons, orbital energies to 0.01 au, and total energies to 0.02 au (all standard deviations), in computational times only a few times larger than those required for complete neglect of differential overlap calculations.

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