X‑ray Crystallographic Characterization of New Soluble Endohedral Fullerenes Utilizing the Popular C<sub>82</sub> Bucky Cage. Isolation and Structural Characterization of Sm@<i>C</i><sub>3<i>v</i></sub>(7)‑C<sub>82</sub>, Sm@<i>C</i><sub><i>s</i></sub>(6)‑C<sub>82</sub>, and Sm@<i>C</i><sub>2</sub>(5)‑C<sub>82</sub>

Abstract

Three isomers of Sm@C<sub>82</sub> that are soluble in organic solvents were obtained from the carbon soot produced by vaporization of hollow carbon rods doped with Sm<sub>2</sub>O<sub>3</sub>/graphite powder in an electric arc. These isomers were numbered as Sm@C<sub>82</sub>(I), Sm@C<sub>82</sub>(II), and Sm@C<sub>82</sub>(III) in order of their elution times from HPLC chromatography on a Buckyprep column with toluene as the eluent. The identities of isomers, Sm@C<sub>82</sub>(I) as Sm@<i>C</i><sub><i>s</i></sub>(6)-C<sub>82</sub>, Sm@C<sub>82</sub>(II) as Sm@<i>C</i><sub>3<i>v</i></sub>(7)-C<sub>82</sub>, and Sm@C<sub>82</sub>(III) as Sm@<i>C</i><sub>2</sub>(5)-C<sub>82</sub>, were determined by single-crystal X-ray diffraction on cocrystals formed with Ni­(octaethylporphyrin). For endohedral fullerenes like La@C<sub>82</sub>, which have three electrons transferred to the cage to produce the M<sup>3+</sup>@(C<sub>82</sub>)<sup>3–</sup> electronic distribution, generally only two soluble isomers (<i>e.g.</i>, La<i>@C</i><sub>2<i>v</i></sub>(9)-C<sub>82</sub> (major) and La@<i>C</i><sub><i>s</i></sub>(6)-C<sub>82</sub> (minor)) are observed. In contrast, with samarium, which generates the M<sup>2+</sup>@(C<sub>82</sub>)<sup>2–</sup> electronic distribution, five soluble isomers of Sm@C<sub>82</sub> have been detected, three in this study, the other two in two related prior studies. The structures of the four Sm@C<sub>82</sub> isomers that are currently established are Sm@<i>C</i><sub>2</sub>(5)-C<sub>82</sub>, Sm@<i>C</i><sub><i>s</i></sub>(6)-C<sub>82</sub>, Sm@<i>C</i><sub>3<i>v</i></sub>(7)-C<sub>82</sub>, and Sm@<i>C</i><sub>2<i>v</i></sub>(9)-C<sub>82</sub>. All of these isomers obey the isolated pentagon rule (IPR) and are sequentially interconvertable through Stone–Wales transformations

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