Aromatic stacking of nucleic acid bases is one of the key players in determ
ining the structure and dynamics of nucleic acids. The arrangement of nucle
ic acid bases with extensive overlap of their aromatic rings gave rise to n
umerous often contradictory suggestions about the physical origins of stack
ing and the possible role of delocalized electrons in stacked aromatic pi.
systems, leading to some confusion about the issue. The recent advance of c
omputer hardware and software finally allowed the application of state of t
he art quantum-mechanical approaches with inclusion of electron correlation
effects to study aromatic base stacking, now providing an ultimitate quali
tative description of the phenomenon. Base stacking is determined by an int
erplay of the three most commonly encountered molecular interactions: dispe
rsion attraction, electrostatic interaction, and short-range repulsion. Unu
sual (aromatic-stacking specific) energy contributions were in fact not evi
denced and are not necessary to describe stacking. The currently used simpl
e empirical potential form, relying on atom-centered constant point charges
and Lennard-Jones van der Waals; terms, is entirely able to reproduce the
essential features of base stacking. Thus, we can conclude that base stacki
ng is in principle one of the best described interactions in current molecu
lar modeling and it allows to study base stacking in DNA using large-scale
classical molecular dynamics simulations. Neglect of cooperativity of stack
ing appears to be the most serious approximation of the currently used forc
e field form.
This review summarizes recent developments in the field. It is written for
an audience that is not necessarily expert in computational quantum chemist
ry and follows up on our previous contribution (Sponer et. al., J. Biomol.
Struct. Dyn. 14, 117, (1996)). First, the applied methodology, its accuracy
, and the physical nature of base stacking is briefly overviewed, including
a comment on the accuracy of other molecular orbital methods and force fie
lds. Then, base stacking is contrasted with hydrogen bonding, the other dom
inant force in nucleic acid structure. The sequence dependence and cooperat
ivity of base stacking is commented on, and finally a brief introduction in
to recent progress in large-scale molecular dynamics simulations of nucleic
acids is provided. Using four stranded DNA assemblies as an example, we de
monstrate the efficacy of current molecular dynamics techniques that utiliz
e refined and verified force fields in the study of stacking in nucleic aci
d molecules.