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85034515910
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note
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We used the standard ADF basis sets IV (Fe) and V (C, O, and H). These are uncontracted triple-ζ valence basis sets that contain one (Fe) or two (C, O, H) sets of polarization functions. The atomic orbitals up to and including the 2p shell on Fe, and the 1s shell on O and C were considered as core and treated by the frozen core approximation (Ref. 58). A set of auxilary s, p, d, f, and g STO functions, centered on all nuclei, is part of the standard basis sets. It was employed to fit the electron density and to present the density dependent Coulomb and XC potentials accurately in each SCF cycle (Ref. 67).
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MO numbers within a given representation refer to valence MOs only, i.e., frozen core shells (Fe: 1s, 2s, and 2p; C, O: 1s) are excluded (Ref. 68). For consistency, this same MO numbering scheme is also employed for the discussion of GAUSSIAN results - even though these calculations use all electron basis sets.
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81
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85034500544
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(0) if the whole expression Eq. (9) is used, rather than the approximation Eq. (12).
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82
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85034493241
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See Ref. 43, and references cited therein. The derivative discontinuity has, in addition, been discussed by Tozer and Handy (Ref. 83).
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86
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HF energies of occupied MOs are, however, good estimates of the respective ionization potentials, according to Koopman's theorem (Refs. 43-45, 84).
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