posted on 2015-12-17, 00:28authored byBastian Kern, Dmitry Strelnikov, Patrick Weis, Artur Böttcher, Manfred
M. Kappes
C<sub>60</sub><sup>2+</sup> and C<sub>60</sub><sup>3+</sup> were
produced by electron-impact ionization of sublimed C<sub>60</sub> and
charge-state-selectively codeposited onto a gold mirror substrate
held at 5 K together with neon matrix gas containing a few percent
of the electron scavengers CO<sub>2</sub> or CCl<sub>4</sub>. This
procedure limits charge-changing of the incident fullerene projectiles
during matrix isolation. IR, NIR, and UV–vis spectra were then
measured. Ten IR absorptions of C<sub>60</sub><sup>2+</sup> were identified.
C<sub>60</sub><sup>3+</sup> was observed to absorb in the NIR region
close to the known vibronic bands of C<sub>60</sub><sup>+</sup>. UV
spectra of C<sub>60</sub>, C<sub>60</sub><sup>+</sup>, and C<sub>60</sub><sup>2+</sup> were almost indistinguishable, consistent with a plasmon-like
nature of their UV absorptions. The measurements were supported by
DFT and TDDFT calculations, revealing that C<sub>60</sub><sup>2+</sup> has a singlet <i>D</i><sub>5<i>d</i></sub> ground
state whereas C<sub>60</sub><sup>3+</sup> forms a doublet of <i>C</i><sub><i>i</i></sub> symmetry. The new results
may be of interest regarding the presence of C<sub>60</sub><sup>2+</sup> and C<sub>60</sub><sup>3+</sup> in space.