Accompanying the rapidly growing
list of σ-hole bonds has
come the acknowledgment of parallel sorts of noncovalent bonds which
owe their stability in large part to a deficiency of electron density
in the area above the molecular plane, known as a π-hole. The
origins of these π-holes are probed for a wide series of molecules,
comprising halogen, chalcogen, pnicogen, tetrel, aerogen, and spodium
bonds. Much like in the case of their σ-hole counterparts, formation
of the internal covalent π-bond in the Lewis acid molecule pulls
density toward the bond midpoint and away from its extremities. This
depletion of density above the central atom is amplified by an electron-withdrawing
substituent. At the same time, the amplitude of the π*-orbital
is enhanced in the region of the density-depleted π-hole, facilitating
a better overlap with the nucleophile’s lone pair orbital and
a stabilizing n → π* charge transfer. The presence of
lone pairs on the central atom acts to attenuate the π-hole
and shift its position somewhat, resulting in an overall weakening
of the π-hole bond. There is a tendency for π-hole bonds
to include a higher fraction of induction energy than σ-bonds
with proportionately smaller electrostatic and dispersion components,
but this distinction is less a product of the σ- or π-character
and more a function of the overall bond strength.