The wave function of a system may be expanded in terms of eigenfunctions of the N -1 electron Hamiltonian times one-particle functions known as generalized overlap amplitudes (GOAS). The one-electron operator whose eigenfunctions are the GOAS is presented, without using an energy-dependent term as i
The extended Koopmans' theorem Fock operator
β Scribed by J. Mauricio O. Matos; Orville W. Day
- Publisher
- John Wiley and Sons
- Year
- 1987
- Tongue
- English
- Weight
- 915 KB
- Volume
- 31
- Category
- Article
- ISSN
- 0020-7608
No coin nor oath required. For personal study only.
π SIMILAR VOLUMES
Thhe ex.tendcd'Koopmans' theorem eiSenvalues of a correlnted ground state are shown to represent the ccntroids of groups of ionization processes in the sudden limit. Lowest order rehxstion effects are nbscnt.
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 Koopman
## Abstract The extended Koopmans' theorem has been implemented using multiconfigurational selfβconsistent field wave functions calculated with the GAMESS, HONDO, and SIRIUS programs. The results of illustrative calculations are presented for the molecules HF, H~2~O, NH~3~, CH~4~, N~2~, CO, HNC, HC