The superexchange interactions between the fullerenes arise as a result of the electron transfer from the C60 molecule to the alkali atom and back. We present a scheme, which is a configuration interaction approach based on the valence bond (Heitler‐London) method. The effect of superexchange is described together with chemical bonding by constructing and solving a secular equation, rather than by using a perturbation treatment. We have considered 180° and 90° superexchange for the C60‐Cs‐C60 pathways. The calculations account for unusual electronic properties of polymer orthorhombic and quenched cubic phases of CsC60: two lines in nuclear magnetic resonance experiments, the development of a spin‐singlet ground state and a decrease of magnetic susceptibility as T→0.

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