The motion of the C2 dumbbells in K2C2 in the low-temperature (LT-K2C2, I41/acd, Z
= 8) and high-temperature (HT-K2C2, Fmm, Z
= 4) modifications was examined by a combination of synchrotron powder diffraction and 13C solid-state NMR spectroscopy. For LT-K2C2, the experimental data are consistent with a motion restricted to a double cone with the cone angle becoming wider with increasing temperature. In HT-K2C2, the C2 dumbbells are less restricted and undergo a fast reorientation that averages out the large chemical shift anisotropy (292 ppm) found in LT-K2C2. Hence, the disorder observed in XRPD experiments is caused by this dynamic process with a characteristic time constant much shorter than 4 μs. However, a distinction between an isotropic free rotation (Pauling model) and a random exchange process between distinct directions consistent with cubic symmetry (Frenkel model) is not possible on the basis of the experimental data obtained.
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