1961
DOI: 10.1090/s0025-5718-1961-0129566-x
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An improved eigenvalue corrector formula for solving the Schrödinger equation for central fields

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Cited by 409 publications
(320 citation statements)
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“…In CASSCF, the active space was composed by the valence molecular orbitals (MOs) of N 2 to which we added one σ g and one π g MOs for better relaxation of the wavefunctions of the N 2 electronic states whose configurations differ in their σ π orbital occupations. We used an active space larger than the valence and a diffuse basis set in order to well describe any possible The nuclear motion problem was solved using the method of Cooley [29]. The spectroscopic constants discussed below were obtained using the derivatives at the minimum energy distances and standard perturbation theory.…”
Section: Methodsmentioning
confidence: 99%
“…In CASSCF, the active space was composed by the valence molecular orbitals (MOs) of N 2 to which we added one σ g and one π g MOs for better relaxation of the wavefunctions of the N 2 electronic states whose configurations differ in their σ π orbital occupations. We used an active space larger than the valence and a diffuse basis set in order to well describe any possible The nuclear motion problem was solved using the method of Cooley [29]. The spectroscopic constants discussed below were obtained using the derivatives at the minimum energy distances and standard perturbation theory.…”
Section: Methodsmentioning
confidence: 99%
“…The wave functions were obtained numerically using the standard Numerov method [26,27,28] with a step size of 0.001 a 0 over internuclear distances 0.1 < R < 200 a 0 .…”
Section: Photodissociation Approachmentioning
confidence: 99%
“…In TROVE, the primitive vibrational basis set is represented by a symmetrized product of six one-dimensional vibrational functions φn 1 (r ℓ 1 ), φn 2 (r ℓ 2 ), φn 3 (r ℓ 3 ), φn 4 (θ ℓ 1 ), φn 5 (θ ℓ 2 ), and φn 6 (τ ), where ni denotes the associated local mode vibrational quanta, {r ℓ 1 , r ℓ 2 , r ℓ 3 , θ ℓ 1 , θ ℓ 2 } are linearized versions (Yurchenko et al 2007;Bunker & Jensen 1998) of the coordinates {rCO, rCH 1 , rCH 2 , θOCH 1 , and θOCH 2 }, respectively, and τ is the dihedral angle between the OCH1 and OCH2 planes. The functions φn i (qi) are obtained by solving the corresponding 1D Schrödinger equation (Yurchenko et al 2007) for the vibrational motion associated with the corresponding coordinate qi ∈ {r ℓ 1 , r ℓ 2 , r ℓ 3 , θ ℓ 1 , θ ℓ 2 , τ }, with the other coordinates held fixed at their equilibrium values, where the Numerov-Cooley method (Noumerov 1924;Cooley 1961) is used. The direct product of the 1D basis functions is contracted using the polyad condition:…”
Section: Variational Computationmentioning
confidence: 99%