Upon examination of the bond distances of the recently reported series of [Ln(SST) 3 (THF) 2 ] [Ln = lanthanides, SST = tris(trimethylsilyl)siloxide (OSi(SiMe 3 ) 3 ), and THF = tetrahydrofuran] compounds, it was found that over the Ln-series (La through Lu), the Ln−O(THF) bond changed by 0.257 Å, whereas the Ln−O(SST) bond varied by 0.164 Å. Examination of all similarly ligated Ln−O(THF) (Ln = La vs Lu) structures available in the Cambridge Structural Database (CSD) revealed that this previously unreported, increased Ln-contraction is pervasive. Further evaluations showed that this enhanced Lncontraction also occurs for pyridine (py) in the [Ln(SST) 3 (py) 2 ] family as well as the average Ln−N(py) (La vs Lu) structure distances recovered from the CSD. Additional ligands, such as halides (Cl and I) were found to display this enhanced Lncontraction, while other species (i.e., cyclopentadienide, alkoxide, SST, and dimethyl sulfoxide) yielded a "normal" Ln-contraction (La−L vs Lu−L). Gas-phase electronic structure density functional theory calculations were carried out to evaluate the molecular orbital influence on the Ln-contraction between Ln−O(SST) and Ln−O(THF). The calculated [Ln(SST) 3 (THF) 2 ] structures were found to demonstrate the same capricious Ln-contraction. Based on these studies, one can say that the variability of the Lncontraction noted in the [Ln(SST) 3 (THF) 2 ] experimental data is due to the different bonding types, ion−ion for the Ln−SST bond versus ion−dipole for the Ln−THF bond.