X-ray crystallographic studies, low-temperature X H and 13C NMR studies, and 27Al NMR studies of a series of homoleptic tricyclopentadienylalum inum compounds [(CßHs^Al (1 ), (MeCßHJsAl (2 ), ( l,2 ,4 -Me3C5H2)3Al (3), ( l , 2 ,3 ,4*Me4C5H )3Al (4)] are reported along w ith ab initio calculations on model cyclopentadienylaluminum compounds. The ring-coordination geometries exhibited by the tricyclopentadienylaluminum compounds in the solid state vary with the number of methyl substituents on the cyclopentadienyl rings. The X-ray crystal structure of compound 1 revealed two unique m olecules in the unit cell, one w ith an {rf, rji'5, rf3} combination of ring geometries and the other w ith an {t/2, j/1* 6, rj1} combination of ring-coordination geometries. In the crystal structure of compound 3, one cyclopentadienyl ring is coordinated rf to the aluminum while the other two rings are if. Compound 4 exhibits monohapto coordination of all three tetram ethyl-substituted cyclopentadienyl rings in the solid state. These compounds are highly fluxional in solution and exhibit averaged 1H and 13C NMR spectra in the fast-exchange limit at temperatures as low as -1 1 0 °C. This behavior is explained by the ab initio calculations on model cyclopentadienylalum inum compounds which reveal almost negligible (1 -2 kcal/mol) energy differences betw een different ring hapticities (i;1, rf, rf, rf).
Introduction
«The cyclopentadienyl ligand is probably best known for its pentahapto-coordination geometiy with transition metals. In the absence of accessible d orbitals, jr-type interactions are weaker, and deviation from 775-geometry by "ring slippage" is often observed. These "ringslipped" (rj1, rf¡ if) structures are more commonly observed among the cyclopentadienyl-main-groupmetal compounds.1" 3 Along with these ring-slipped geometries, cyclopentadienyl compounds of the maingroup elements exhibit varying degrees of fluxionality. Two different sigmatropic processes have been identified experimentally for a-bonded (rj1) species, a 1 ,2-hydrogen shift and a 1,2-shift of the main-group element.4 De tailed mechanistic information on these systems has been obtained, where possible, with the help of variable temper ature NMR techniques.In the case of aluminum, rearrangements are too fast at accessible temperatures to be monitored by NMR. Moreover, equilibrium structures are frequently not rf but ?;L5, rf, or rf> which complicates the discussion of "the sigmatropic process". Nevertheless, it has gener ally been assumed, by extrapolation from experimen tally characterizable systems, that a similar "ringwhizzing"5-8 mechanism is responsible for the dynamic behavior observed in the X H and 13C NMR spectra of cyclopentadienylaluminum compounds. Gas-phase elee-