Pc. Hiberty et al., WHY DOES BENZENE POSSESS A D-6H SYMMETRY - A QUASI-CLASSICAL STATE APPROACH FOR PROBING PI-BONDING AND DELOCALIZATION ENERGIES, Journal of the American Chemical Society, 117(29), 1995, pp. 7760-7768
In response to a recent controversy over the issue of whether the pi-e
lectrons of benzene do or do not possess a distortive tendency away fr
om a D-6h symmetry, we have developed a new approach based on the quas
iclassical (QC) state, which is the spin-alternant state of a chemical
species and which allows definition of the pi-bonding energy in a man
ner which does not depend on energy partition and is free of the dilem
ma of assignment of the nuclear repulsion. The QC state concept is app
lied to probe bonding energies in H-2 and C2H4 and then used to quanti
fy delocalization energies of H-6 and benzene. It is shown that the pi
-bonding energy of benzene is stabilized by a localizing B-2u distorti
on. As such, the pi-system of benzene behaves precisely like the deloc
alized Hg hexagon which is a transition state more stable in a distort
ed D-3h geometry. The analogy between the delocalized pi-electrons of
benzene and H-6 is further highlighted by demonstrating, computational
ly, that they both possess exalted diamagnetic susceptibilities associ
ated with ring currents. While H-6 simply falls apart to three H-2 mol
ecules, the pi-electrons of benzene are held together by the sigma-fra
me. Benzene is therefore the site of two opposing driving forces. The
pi driving force tends to distort the molecule while the stronger a dr
iving force of the QC state acts in the opposite direction and imposes
a regular geometry. As such, benzene possesses a unique delocalized p
i-component which has a dual nature; at any geometry of the C6H6 struc
ture, the pi-electrons are strongly stabilized by the quantum mechanic
al resonance energy (QMRE), and at the same time, they possess a globa
l distortive tendency toward a D-3h structure. It is demonstrated that
this dual picture of benzene is in perfect agreement with the ''aroma
tic'' behavior of benzene. Applications are presented to the Stanger m
odel of bent benzene, tricyclobutabenzene, and naphthalene.