Asbrink and co-rvorkers claim that in CRcu HA&'3 Inethod the correlation energy ant1 the self-repuleion are trestcd carrccily. Their claims arc criticzlly cuamincd.
HAM/3, a semi-empirical MO theory. I. The SCF method
✍ Scribed by L. Åsbrink; C. Fridh; E. Lindholm
- Publisher
- Elsevier Science
- Year
- 1977
- Tongue
- English
- Weight
- 644 KB
- Volume
- 52
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
✦ Synopsis
An MO SW theory for molecules hd~ been dcvclopcd startmg from Slatcr's study of atonlac 4liclding constants USC of shielding "constants" which are frlrzctions of the nature of the shielded electron glvcs good total cncrgics for a number of atomic species. The good :isecment must mean negligible errors due to correl,ition and \elf-repulsion. To c?rtend this treatment to molecules the relation FflV = X/aPgV is used. The proccdurc hag been pnramctrbcd tar H. C, N, 0 'md l-.
📜 SIMILAR VOLUMES
Photoelectron spectra of benzene, pyridinc, cthylcnc, aone and butiidiene are cAculated by USC of tbc MO SCF method HAM/3. Since the correlation energy errors ~cem to be negligible in this method, Koopmane' theorem cannot be used. Instead, a transitIon state procedure is used. The calculations are c
## Electron affhttcs and excitntion cnergm for benrenc. pyridmc, ethylene. ozone, butacfiene and cyclapropane are catcufnted by 1iFe of the MO SW mctflod HAM/3. %xX? in tf11s method the sclfzrcpulsion Seems to bc complctcly eliminated, the unoccupied orbit& hve corrwt cnerglcb, aid tfwefore the av