The ongoing pursuit of weakly coordinating anions [1] (WCAs) has allowed the synthesis, isolation, and catalytic utilization of highly electrophilic transition-metal [2] and main-group [3] À . [4,5] While a truly noncoordinating anion has not been identified, there is little doubt that this class of anion has been a wellspring of both fundamental insights and industrial applications. [6] During our studies of sterically expanded single-site catalysts for olefin polymerization, [7] we observed consistent trends indicating that increased steric bulk around the electrophilic transition metal yielded increased catalytic activity, for both metallocene catalysts ( Figure 1) and constrained-geometry catalysts (CGCs).[8] These observations are reminiscent of the increased activities observed with increasingly non-coordinating anions, but they must have a different root cause, as the same methylaluminoxane (MAO)-derived counteranion was common among these polymerizations.We postulated that the increased activity was a result of steric shielding effected by the expanded ancillary ligands; this steric sheath diminished the ability of the encased electrophilic metal center to accept the larger counteranion, but it still allowed access to the relatively small monomers. Figure 2 illustrates how steric bulk might retard the accepting ability of such electrophiles, resulting in what should be weakly coordinating cations (WCCs).[9] We then sought additional evidence to test this supposition and turned our attention to UV/Vis spectroscopy. [10] Upon activation with MAO (5000 equiv), zirconocene [{Ph 2 C(C 5 H 4 )(C 13 H 8 )}ZrCl 2 ] (1-Flu) undergoes an immediate red shift of its visible absorption maximum l max from 499 to 557 nm (DE = À5.97 kcal mol À1 = À25.0 kJ mol À1 ). Zirconocene [{Ph 2 C(C 5 H 4 )(C 29 H 36 )}ZrCl 2 ] (1-Oct) also undergoes a rapid red shift, but of significantly greater magnitude: 521 to 622 nm (DE = À8.91 kcal mol À1 = À37.3 kJ mol À1 ). For these species, l max corresponds to a ligand-to-metal charge transfer (LMCT), [10a, 11] and the change in l max upon MAO activation is a direct measure of the resultant electron density at the zirconium center, because the LMCT is correspondingly more facile for more electron-deficient metals. Thus, the zirconocenium ion pair generated from 1-Oct features a more electron-deficient metal center, and a plausible explanation for this electron deficiency is a greater average cation-anion separation caused by steric shielding (Figure 2).Over the course of 3 h, the l max of activated 1-Oct relaxes back to 590 nm, while the l max of activated 1-Flu remains unchanged at 557 nm. Figure 3 plots this dynamic process and