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Laser vaporization experiments with graphite in a supersonic cluster beam apparatus indicate that the smallest fullerene to form in substantial abundance is C(28). Although ab initio quantum chemical calculations predict that this cluster will favor a tetrahedral cage structure, it is electronically open shell. Further calculations reveal that C(28) in this structure should behave as a sort of hollow superatom with an effective valence of 4. This tetravalence should be exhibited toward chemical bonding both on the outside and on the inside of the cage. Thus, stable closed-shell derivatives of C(28) with large highest occupied molecular orbital-lowest unoccupied molecular orbital gaps should be attainable either by reacting at the four tetrahedral vertices on the outside of the C(28) cage to make, for example, C(28)H(4), or by trapping a tetravalent atom inside the cage to make endothedral fullerenes such as Ti@C(28). An example of this second, inside route to C(28) stabilization is reported here: the laser and carbon-arc production of U@C(28).

Buckminsterfullerene, c60, was prepared in gram quantities by contact-arc vaporization of a graphite rod in a 100-Torr atinospherc of helium. followed by extraction of the resultant graphitic soot with toluene. The dominance of C , in this extract was verified by mass, FTIR. and NMR spectroscopy. The molecule was successfully hydrogenated to C6,H,, via a Birch reduction and dehydrogenated back to bare c 6 0 by treatment with DDQ reagent. Cyclic voltammetry of C60 in methylene chloride rcvcaled highly reversible formation of at least two stable anionic forms of c 6 0 in solution. A broad new class of thcsc fulleride and fulleronium ions is anticipated, both with the internal cavity empty and with any one of a large number of elcmcnts inside, thus providing a means of fine-tuning the chemical, optical, and redox properties.

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