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>
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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