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Salts of fullerene C60˙- and endometallofullerene Sc3N@Ih-C80˙- radical anions with Bu3MeP+ cations ((Bu3MeP+)3(C60˙-)3·C6H4Cl2 (1) and (Bu3MeP+)3(Sc3N@Ih-C80˙-)3·C6H4Cl2 (2)) have been obtained. The C3 symmetry of the Bu3MeP+ cation provides 2D Kagome lattices with an equilateral triangle arrangement of fullerenes in accordance with trigonal crystal symmetry P31m. The C60˙- and Sc3N@Ih-C80˙- radical anions preserve their monomeric forms in 1 and 2 with the S = 1/2 spin state down to 1.9 K. The close packing of the fullerene radical anions results in strong antiferromagnetic coupling of the spins with Weiss temperatures of -108 K for 1 and -43 K for 2. Compound 1 is a rare example of a magnetic system in which in spite of the strong magnetic coupling of spins no long-range ordering is observed down to 1.9 K. The 13C NMR spectra of the 13C enriched sample of 1 support the absence of the antiferromagnetic ordering of spins down to 1.5 K. Thus, the crystals of 1 preserve large spin frustration forced by the trigonal symmetry. Therefore, compound 1 is a promising candidate for the first observation of a quantum spin liquid (QSL) state in a fullerene-based system. Isostructural salt 2 is the first compound that contains monomeric paramagnetic Sc3N@Ih-C80˙- radical anions stable down to 1.9 K, which show strong spin frustration. These data indicate the ability of endometallofullerenes to give exotic magnetic systems such as QSLs.

New fullerene salts (TMP(+))2·(C60(2-))·(C6H4Cl2)2 (1), {DB-18-crown-6·[Na(+)]·(C6H5CN)2}2·(C60(2-))·C6H5CN·C6H4Cl2 (2), {cryptand[2,2,2]·(Na(+))}2·(C60(2-)) (3) and (PPN(+))2·(C60(2-))·(C6H4Cl2)2 (4) were obtained as single crystals. Their crystal structures were solved and their optical and magnetic properties were analyzed. The spectra of the salts in the IR and UV-visible-NIR ranges indicate the formation of C60(2-) dianions in 1-4. These salts show similar behavior in EPR measurements, explained by the diamagnetic ground state of the C60(2-) dianions and the thermal population of the excited triplet state, which is separated by an energy gap of 487-540 cm(-1). The magnetic susceptibility of 4 also increased above 130 K due to the population of the excited triplet state. The observed splitting of the C60 LUMO is attributed to the Jahn-Teller (JT) effect. We analyzed the splitting by an extended Hückel method using the single-crystal structural data for the compounds containing neutral, mono- and dianions of C60. The splitting of the initially triply degenerated C60 LUMO produces three molecular orbitals. The gap between the lowest and highest orbitals is very small in neutral C60 (128-140 cm(-1)), it increases in C60(˙-) (500-710 cm(-1)) and increases further in C60(2-) (1080-1670 cm(-1)). It was found that the splitting of the C60 LUMO is realized in different ways for the mono- and dianions. The ground and first excited state are separated in C60(˙-) by a small gap of 55-180 cm(-1) only. This gap is noticeably larger in the C60(2-) dianions and falls into the 760-1390 cm(-1) range.