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In II and III, we have tried to determine with X-rays toward the low temperatures whether these rotations of the t-Bu groups and the movements of the methyl carbons of the counterions become blocked. In effect, at 90 K, the two compounds present a new phase and a different structure of lower symmetry than that observed at 300 K. This structure is fairly complicated (probably triclinic but with α, β, and γ angles very close to 90°), and it probably contains a large number of inequivalent molecules. We have been unable to solve it without ambiguity. The change from this low-symmetry phase to the phase described at room temperature occurs at ∼120-130 K for II and ∼150-160 K for III. Therefore, these X-ray observations confirm that the movements-in the solid state and especially the rotations of the t-Bu groups of the thiolate ligands are operative in the whole range of temperatures where we perform these solid-state NMR experiments.
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2 carbon p orbital pointing toward the thiolate sulfur bears some spin density leading to a non-negligible anisotropy contribution, we took this term explicitly into account, evaluating its relative weight from density functional calculations, in a manner described elsewhere. This is in contrast to the proton case, whose s Orbitals do not allow for some local source of dipolar anisotropy. Results to be published.
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