The present review is aimed to compare
crystal packing interactions
contributing to stacking arrangements of primarily nonaromatic systems
referring only briefly to classical aromatic stacking. The classical
aromatic stacking is mainly based on weak dispersion interactions
(E ≤ 1 kcal mol–1) whereas
heteroaromatics reveal more electrostatic (or specifically dipolar)
contributions (E = 5–10 kcal mol–1). Based mainly on our charge density studies and DFT calculations,
the results show that (i) all planar rings stack, regardless of aromaticity
(or delocalization of π electrons) and (ii) stacking interactions
cover a wide continuum ranging from weak, mainly dispersion interactions
(E < 5 kcal mol–1) to unlocalized
two-electron multicentric (2e/mc) covalent bonds (“pancake
bonds”, E > 15 kcal mol–1). Our recent studies showed that quinones form face-to-face stacks
and the energies of interactions exceed 10 kcal mol–1; ours and other authors’ results indicate that interactions
between planar radicals involve a significant contribution of covalent
bonding. Thus, π-interactions cover a broad range of energies,
ranging from ≤1 to ≥20 kcal mol–1,
and the interactions span from weak dispersion to multicentric covalent
bonding. Therefore, development of a universal model of stacking is
needed. In this respect, stacking can be compared to hydrogen bonding,
which also ranges between dispersion (weakest hydrogen bonds, such
as C–H···S and C–H···Cl)
and two-electron/three-centric covalent bonding (the strongest “symmetrical”
hydrogen bonds).