Solvent interaction within the Hartree-Fock SCF molecular orbital formalism

1974 ◽  
Vol 34 (2) ◽  
pp. 145-155 ◽  
Author(s):  
Henry A. Germer
1991 ◽  
Vol 95 (10) ◽  
pp. 7466-7478 ◽  
Author(s):  
Neil A. Burton ◽  
Yukio Yamaguchi ◽  
Ian L. Alberts ◽  
Henry F. Schaefer

1982 ◽  
Vol 60 (17) ◽  
pp. 2281-2285 ◽  
Author(s):  
Milan Trsic ◽  
William G. Laidlaw ◽  
Richard T. Oakley

Abinitio Hartree–Fock–Slater molecular orbital calculations on the planar tetrasulphur tetranitride dication S4N42+ reveal that it can be described as a fully delocalised 10 π-electron system. Overlap populations for the NS bonds suggest a bond order substantially stronger than in neutral S4N4. The strong uv/visible absorptions observed for S4N42+ at 346 and 262 nm are assigned to nπS → π* and nπN → π* excitations. The Hartree–Fock–Slater π-molecular orbital manifold is discussed in relation to simple HMO concepts.


2000 ◽  
Vol 55 (9-10) ◽  
pp. 769-771 ◽  

Abstract Molecular orbital calculations were performed for the six saturated alkylamines (CH3NH2 , (CH3)2 NH, (CH 3)3 N, CH 3CH2NH2 , (CH3)2 CHNH2 , (CH3)3 CNH2), their protonated cations (CH3NH3 + , (CH3)2NH2 + , (CH3)3NH + , CH3CH2NH3 + , (CH3)2CHNH3 + , (CH3)3CNH3+), and (CH3)4 N + using the Hartree-Fock, second-order M0ller-Plesset, and density functional theory methods with the 6-311+G(d,p) basis set. Protonation lengthens the C-N bonds of the amines by 0.05 -0.08 Å and shortens the C-C bonds of CH3CH2NH2, (CH3)2CHNH2 , and (CH3)3CNH2 by ca. 0.01 Å.


1965 ◽  
Vol 53 (5) ◽  
pp. 1089-1091 ◽  
Author(s):  
M. D. Newton ◽  
F. P. Boer ◽  
W. E. Palke ◽  
W. N. Lipscomb

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