All 19 Isolated‐Pentagon‐Rule isomers of fullerene C 86 were investigated by Density Functional Theory (DFT) methods with B3LYP functional at 6‐31G, 6‐31G*, and 6‐31+G* levels. Preliminary distribution of single, double, and delocalized pi‐bonds in molecules of these isomers of fullerene C 86 is fulfilled. Obtained results are perfectly supported by DFT quantum–chemical calculations of electronic and geometrical structures of these isomers. The main reason of instability of isomers 1, 3–15, 18, and 19 are phenalenyl‐radical substructures. Thus, there is a possibility to obtain them only as endohedral metallofullerenes or exohedral derivatives. Isomer 2 (C 2 ) is unstable due to higher local molecular strain. It is shown that empty C 86 may be produced and extracted only as isomers 16 (C s ) and 17 (C 2 ).
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Khamatgalimov et al. (2010) studied this question.
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