For a closed-shell MO conr~gurar~on =I& 2n ck~rons v.hlch occupy n non-degsnrraw canomcal MO> 11 I\ dr'duced that the RHF energy X:\_,[Zf/:: +Z;\_,(2J,, -K,,)] may br expressed m Huchel-hhr form as 2X:'\_ ,c, = -r:\_,[f,(x + I)+ I,(h + 2)] wth A = 2(n -I) The I,(h + 1) and 1,(X +2) are the mmzwon po
Orbital energies and Koopmans' theorem in open-shell Hartree-Fock theory
✍ Scribed by J.L. Dodds; R. McWeeny
- Publisher
- Elsevier Science
- Year
- 1972
- Tongue
- English
- Weight
- 455 KB
- Volume
- 13
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
✦ Synopsis
In (restricted) open-shell Hartree-Fock theory, the ebenvalues of the effective hamiltonian do not have the &al significance as negative jonization potentials (Koopmans' theorem). By defii orbital energies in terms of certain en-. ergyexpectation values, it is possible to obtain analogues of Koopmans' theorem, and to discuss the energetics of
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