1991
DOI: 10.1016/0010-4655(91)90139-c
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A configuration interaction program

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Cited by 64 publications
(48 citation statements)
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“…In the second step one calculates the electron correlation energy in terms of the orbitals from the first step, in particular by considering excitations (or de‐excitations) of one, two, three, or more electrons from occupied orbitals in the reference function to various unoccupied orbitals. A key issue in such calculations is whether the reference function consists of a single configuration state function129, 131–133 (CSF) or a linear combination of two or more CSFs,13, 43, 84, 91, 120, 129, 134–140 where a CSF is an antisymmetric many‐electron trial wave function composed (usually) of the minimum number of Slater determinants required to obtain the correct spatial and spin symmetry. Calculations in which the reference functions are single CSFs (such as Hartree–Fock wave functions) are called single‐reference methods,129, 131–133 and calculations in which the reference functions consist of multiple CSFs are called multi‐reference methods 13, 43, 84, 91, 120, 129, 134–136…”
Section: Quantum Mechanical Description Of Chemical Bondingmentioning
confidence: 99%
“…In the second step one calculates the electron correlation energy in terms of the orbitals from the first step, in particular by considering excitations (or de‐excitations) of one, two, three, or more electrons from occupied orbitals in the reference function to various unoccupied orbitals. A key issue in such calculations is whether the reference function consists of a single configuration state function129, 131–133 (CSF) or a linear combination of two or more CSFs,13, 43, 84, 91, 120, 129, 134–140 where a CSF is an antisymmetric many‐electron trial wave function composed (usually) of the minimum number of Slater determinants required to obtain the correct spatial and spin symmetry. Calculations in which the reference functions are single CSFs (such as Hartree–Fock wave functions) are called single‐reference methods,129, 131–133 and calculations in which the reference functions consist of multiple CSFs are called multi‐reference methods 13, 43, 84, 91, 120, 129, 134–136…”
Section: Quantum Mechanical Description Of Chemical Bondingmentioning
confidence: 99%
“…The limitations of Storey et al (2000) calculations were addressed by Tayal (2008), who included 135 levels of the 3s 2 3p, 3s3p 2 , 3s 2 3d, 3p 3 , 3s3p3d, 3p 2 3d, 3s3d 2 , 3p3d 2 , 3s 2 4s, 3s 2 4p and 3s 2 4d configurations. For the calculation of energy levels and the A-values, he adopted the multi-configuration Hartree-Fock (MCHF) codes of Froese-Fischer (1991) and Zatsarinny & Froese-Fischer (1999), while for the scattering process the semi-relativistic R-matrix code of Berrington, Eissner & Norrington (1995) was used. Furthermore, he calculated values of Ω up to an energy of 150 Ryd, although the range of partial waves adopted (J 25) is insufficient at higher energies, for the convergence of the allowed and some of the forbidden transitions.…”
Section: Introductionmentioning
confidence: 99%
“…Froese Fischer [64] The MCHF atomic structure package Methods Froese Fischer [65] MCHF support libraries and utilities Package Froese Fischer, Liu [66] Configuration-state lists Package Hibbert, Froese Fischer [67] Angular integrals with non-orthogonal orbitals Package Froese Fischer [68] General MCHF program Package Hibbert, Glass, Froese Fischer [69] Angular integrals for Breit-Pauli Hamiltonian Package Froese Fischer [70] General CI program Package Froese Fischer, Godefroid, Hibbert [71] Angular integrals for transition operators Package Froese Fischer, Godefroid [72] Programs for LS and LSJ transitions Package…”
Section: Short Title Type Of Papermentioning
confidence: 99%