Polycrystalline C-60 has been intercalated with 99 atom % C-13-enriched CO
gas by using high-pressure, high-temperature synthesis. The ratio of (CO)-C
-13 to C-60 is determined using C-13 NMR under magic-angle spinning and is
found to be almost 1:2. Static solid-state C-13 NMR spectra of (CO)-C-13-in
tercalated C-60 have been measured in the range between room temperature an
d 4 K. In the high-temperature range, i.e., between room temperature and 10
0 K, the CO molecules in the "octahedral" sites of the C-60 lattice reorien
t rapidly on the NMR time scale. At 4 K the reorientation rate of CO is so
low that, on the NMR time scale, the molecule appears localized in one of t
he minima of the potential. Between LC and 30 K, the transition from the st
atic to the dynamic regime can be inferred from NMR line shape changes. The
temperature dependence of the line shape is modeled in terms of thermally
activated jump-like reorientations of the CO molecules in the C-60 lattice.
No evidence for a quantum mechanical coherent tunneling motion of the CO m
olecules in the octahedral sites of the C-60 lattice has been found.