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The intermolecular interactions in alkali-doped C60 solids, A3-x-yA’xA“yC60(A, A’, A” =alkali; x + y ≤3), have been calculated, and their correlations with the structures and the superconducting transition temperaturesTc have also been investigated. It is found that the variations of the lattice constants a0 of A3-x-yA’x A“yC60 solids and the superconducting transition temperatures Tc can be satisfactorily explained from the viewpoint of interaction. It is shown that the relationship of Tc with interaction is much closer than that of Tc with lattice constant a0. Therefore, we can say it is the physical factors such as interaction, other than the geometrical structure factors such as a0, that should be reasonably taken as the primitive cause of the sudden change of superconductivity from pristine C60 to its alkali-doped compounds and of the variation of Tc among superconductors of A3-x-yA’xA’yC60.
The intermolecular interactions in alkali-doped C60 solids, A3-x-yA’xA ”yC60 (A, A ’, A “ = alkali; x + y ≦ 3) have been calculated, and their correlations with the structures and the superconducting transition temperaturesTc have also been investigated. It is found that the variations of the lattice constants a0 of A3-x-yA’x A ”yC60 solids and the superconducting transition temperatures Tc can be satisfactorily explained from the viewpoint of interaction. It. is shown that the relationship of Tc with interaction is much closer than that of Tc with lattice constant a0. Therefore, we can say it is the physical factors such as interaction, other than the geometrical structure factors such as a0 as the primitive cause of the sudden change of superconductivity from pristine C60 to its alkali-doped compounds and of the variation of Tc among superconductors of A3-x-yA’xA’yC60.