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Inversion Barrier of Corannulene. A Benchmark for Bowl-to-Bowl Inversions in Fullerene Fragments
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Citations
29
References
1999
Year
Bowl-to-bowl InversionsMolecular SolidEngineeringPhysicsNatural SciencesFullerenePhysical ChemistryGibbs EnergyInversion BarriersComputational ChemistryInversion BarrierQuantum ChemistryChemistryBowl-to-bowl Inversion BarrierAb-initio MethodFullerene Fragments
In a systematic ab initio study, the Hartree-Fock, B3LYP density functional, and MP2 methods are employed to calculate the bowl-to-bowl inversion barrier of corannulene (1). Basis sets ranging from a minimal basis (STO-3G) to a double polarized valence triple-zeta basis (6-311G(2d,2p)) were used. In comparison with experimental data, it was found that inclusion of dynamic electron correlation (e.g., B3LYP) and a 6-311G basis set (or other basis sets with similar complexity) are essential for quantitatively correct results. At B3LYP/6-311G, DeltaG()(298) = 44.9 kJ/mol. Thermal corrections to Gibbs energy of activation were of minor importance in the relevant range of temperatures. Inversion barriers (DeltaE()(Tot)) of the bowl-shaped fullerene fragments C(26)H(12) 4 and C(30)H(12) 5 and the chiral C(30)H(12) 6 are predicted to be 28.0, 199.4, and 277.3 kJ/mol, respectively, at B3LYP/6-311G. Predicted enthalpies of formations and strain energies are also discussed.
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