In this paper we extend the well-known MS Xa method for the calculation of the electronic structure of molecules enclosed in the Watson-sphere to the case of an arbitrarily shaped outer surface. A general formalism is discussed. In r&ent years considerable progress has been made in calculating the
The electronic structure of ionised molecules—VIII: Ethylamine
✍ Scribed by C. Krier; J. C. Lorquet; A. Berlingin
- Publisher
- John Wiley and Sons
- Year
- 1974
- Tongue
- English
- Weight
- 843 KB
- Volume
- 8
- Category
- Article
- ISSN
- 1076-5174
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✦ Synopsis
Abstract
Wavefunctions for the [C~2~H~5~NH~2~]^+^˙ ion in its electronic ground state have been calculated by two variants of the CNDO method. The potential energy surface, the reaction paths, the charge distribution and the overlap populations have been calculated as functions of the internuclear distances in order to elucidate the fragmentation mechanism. The results are compared with the description given by other methods in current use, namely the mechanistic approach and the Hirofa method. The reliability and limitations of the three methods are discussed.
📜 SIMILAR VOLUMES
m final form 9 Notember 1979 lontzatton potenttats of the BrFs and BrFs molecules have been calculated by the SCF DV XCK method. The caiculattons hare been carrted out tn numertwl Hartree-Fock basts sets, or, to be more spectftc. m bases that are extenstons of these bases smce "mutual" bromine Id-fu
Evidence is being presented that F2 has a different type of electronic structure than have Cl2. Br2. as 2s. suggested by the quanticule theory. The internuclear distance, the vibrational force constant and ew changes on excitation for F2 do not agree with those expected for the structures Xt Z2 X"
## Abstract The ionisation energies and the HeI photoelectron spectra of the N‐oxides of diazabenzenes are presented. The valence electronic structures of the N‐oxides are discussed in view of the ionisation energies, and the profiles, of the bands. The interpreted data are compared to calculations
Bc,d = Bd,c= - .