Uniform Localization of Atomic and Molecular Orbitals. I
V. Magnasco, A. Perico
Abstract
V. Magnasco, A. Perico
Abstract
A general procedure for a nonarbitrary external localization of atomic and molecular orbitals given in the form of a general LCAO expansion is introduced by imposing an extremum principle on the sum of certain local orbital populations which are required to be localized in given regions of space, in particular around atoms or between pairs of atoms in the molecule. The localization, which is uniform insofaras these local electron populations are simultaneously maximized in all the available orbitals, yields well-defined inner-shell, lone-pair and bond orbitals. The orthogonal transformation which maximizes the localization function is obtained through an iterative sequence of 2 × 2 rotations between all N (N − 1)/2 possible pairs of molecular orbitals. Convergence was found to be excellent. The method turns out to be exceedingly simple, the coefficients in the LCAO expansion and the overlap integrals between the basic atomic orbitals only being required, and general enough to be valid for the localization of atomic orbitals as well of molecular orbitals, either for exact LCAO—SCF—MO's or for approximate LCAO—MO's constructed from nonorthogonal as well from orthogonal basic sets. The localized orbitals obtained in this paper starting from some unsymmetrically orthogonalized atomic orbitals and from the minimal-basis-set LCAO—SCF—MO wavefunctions given by Ransil for LiH, BH, NH, FH, LiF, BF, CO, Li2, Be2, N2, F2 prove to be very close to the energy localized orbitals recently obtained by Edminston and Ruedenberg by maximizing the sum of the orbital self-repulsion energies.
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A general procedure for a nonarbitrary external localization of atomic and molecular orbitals given in the form of a general LCAO expansion is introduced by imposing an extremum principle on the sum of certain local orbital populations which are required to be localized in given regions of space, in particular around atoms or between pairs of atoms in the molecule. The localization, which is uniform insofaras these local electron populations are simultaneously maximized in all the available orbitals, yields well-defined inner-shell, lone-pair and bond orbitals. The orthogonal transformation which maximizes the localization function is obtained through an iterative sequence of 2 × 2 rotations between all N (N − 1)/2 possible pairs of molecular orbitals. Convergence was found to be excellent. The method turns out to be exceedingly simple, the coefficients in the LCAO expansion and the overlap integrals between the basic atomic orbitals only being required, and general enough to be valid for the localization of atomic orbitals as well of molecular orbitals, either for exact LCAO—SCF—MO's or for approximate LCAO—MO's constructed from nonorthogonal as well from orthogonal basic sets. The localized orbitals obtained in this paper starting from some unsymmetrically orthogonalized atomic orbitals and from the minimal-basis-set LCAO—SCF—MO wavefunctions given by Ransil for LiH, BH, NH, FH, LiF, BF, CO, Li2, Be2, N2, F2 prove to be very close to the energy localized orbitals recently obtained by Edminston and Ruedenberg by maximizing the sum of the orbital self-repulsion energies.
Key concepts: Linear combination of atomic orbitals, Molecular orbital theory, Slater-type orbital, STO-nG basis sets, Basis set, Molecular orbital, Complete active space, Localized molecular orbitals