LCAO-MO-SCF-CI semi-empirical ?-electron calculations on heteroaromatic systems

1967 ◽  
Vol 9 (1) ◽  
pp. 38-50 ◽  
Author(s):  
G. W. Pukanic ◽  
D. R. Forshey ◽  
Br. Jerome D. Wegener ◽  
J. B. Greenshields
Keyword(s):  

1968 ◽  
Vol 9 (4) ◽  
pp. 288-295 ◽  
Author(s):  
D. R. Forshey ◽  
G. W. Pukanic ◽  
Br. Jerome D. Wegener ◽  
J. B. Greenshields
Keyword(s):  


1965 ◽  
Vol 38 (1) ◽  
pp. 83-85 ◽  
Author(s):  
Takeshi Nakajima
Keyword(s):  


1984 ◽  
Vol 37 (4) ◽  
pp. 679 ◽  
Author(s):  
PJ Steenkamp

The relevance of models describing molecular electronic energies including electrostatic as well as covalence effects is outlined and a summary of developments resulting in the present formulation is given. A simple, semi-empirical model based on a LCAO-MO approximation and comprising the point charge electrostatic model and angular overlap model is formulated. Although the present formulation is restricted to the antibonding effects of covalence it is applicable to p, d, f and g orbital energies. The mathematical and conceptual simplicity of the model derives from the application of a re-parameterized ionic model and the superposition principle for ligand contributions, the latter applied in the case of ionic as well as antibonding effects. A physical interpretation of the model, for diatomic as well as polyatomic molecules, is presented and the results of its application to the pentachlorovanadate(IV) ion are cited.





1966 ◽  
Vol 44 (8) ◽  
pp. 1677-1683 ◽  
Author(s):  
P. Felenbok ◽  
H. Lefebvre-Brion

A theoretical interpretation of homogeneous perturbations is proposed for the case of two electronic excited states that differ strongly in electron configuration. The interaction parameter H can be expressed in terms of the vibrational overlap integral and the electrostatic interaction between the two states. In the case of the Π–Π and Δ–Δ interactions in the spectrum of the NO molecule, a semi-empirical calculation of this parameter is made, using Morse functions for the vibrational part and the LCAO-MO SCF function for the electronic part. The comparison with the "experimental" values given by Lagerqvist and Miescher supports this interpretation.



1965 ◽  
Vol 3 (2) ◽  
pp. 147-155 ◽  
Author(s):  
Ricardo Ferreira
Keyword(s):  


1989 ◽  
Vol 185 (1) ◽  
pp. 39-50 ◽  
Author(s):  
Colin F. Bell ◽  
Roger D. Beauchamp ◽  
Eric L. Short


1970 ◽  
Vol 48 (19) ◽  
pp. 2221-2230 ◽  
Author(s):  
S. Jugessur ◽  
J.-Y. Savard ◽  
R. Rai

The semi-empirical LCAO–MO method has been utilized to study the electronic spectra of the Co2+ ion embedded in host crystals of CdS, ZnS, and ZnO. The crystals are assumed to have an axial distortion, thereby changing the Td symmetry to C3v. One-electron energy levels and state vectors are evaluated by the MO method. The results are used to analyze the fine structure of the optical bands of the Co2+ ion in those environments, and to calculate the anisotropic [Formula: see text] and [Formula: see text] and the zero-field splitting D. It is found that the molecular orbitals are good basis functions and that the spin–orbit coupling constant λ, less than the free ion value, is required for a proper assignment of the fine-structure bands.



1974 ◽  
Vol 29 (5) ◽  
pp. 763-767 ◽  
Author(s):  
G. Van Hooydonk

Abstract It is shown how previously reported bond energy equations (Van Hooydonk, 1973) can be regenerated starting from the assumptions (i) that the valence-orbital energy of an element in a bond can be expressed as a function of its occupancy number (Iczkowski-Margrave, 1961) and (ii) that the potential around an atom in a bond vanishes as soon as its valence orbital is doubly occupied (Ferreira, 1963). The results are consistent with an ionic approximation to chemical bonding. A comparison of the approximations involved in the present theory with those in a semi-empirical LCAO -MO method (Klopman, 1964) is advanced.



1976 ◽  
Vol 11 (5) ◽  
pp. 468-471 ◽  
Author(s):  
Heinz Sterk ◽  
Franz Heresch
Keyword(s):  


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