Abstract
Abstract The INDO method has been employed to calculate the isotropic and anisotropic hyperfine interactions for some geometrical structures of the C 6 F 6 − , C 6 HF 5 − , 1,2,4,5-F 4 C 6 H 2 − radical anions. The π and σ states of planar radical anions have been considered together with three types of non-planar structures: (a) with out-of-plane distortions of the benzene ring following the “chair” pattern: (b) with neighbouring fluorine atoms displaced in opposite directions from the ring plane due to their electrostatic repulsion: (c) with symmetric (of type) displacement of CF bonds due to the interaction between the ground and lowest excited σ-electron states within the pseudo-Jahn-Teller effect. It is the last model that describes all experimental data on magnetic resonance parameters. This model is also preferable for energy reasons. Most likely, this type of non-planar structures reflects the basic features of the real geometry of the above radical anions whose ground state may be termed as pseudo-π-electronic since the unpaired electron occupies an orbital that is a linear combination of the π and σ orbitals of the corresponding planar structure with a prevailing π component.
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