Global minimum of the adenine center dot center dot center dot thymine base pair corresponds neither to Watson-Crick nor to Hoogsteen structures. Molecular dynamic/quenching/AMBER and ab initio beyond Hartree-Fock studies
M. Kratochvil et al., Global minimum of the adenine center dot center dot center dot thymine base pair corresponds neither to Watson-Crick nor to Hoogsteen structures. Molecular dynamic/quenching/AMBER and ab initio beyond Hartree-Fock studies, J AM CHEM S, 122(14), 2000, pp. 3495-3499
Computational analysis of complete gas-phase potential energy and free ener
gy surfaces of the adenine thymine base pair has been carried out. The stud
y utilizes a combination of molecular dynamics simulations performed with C
ornell et al. empirical force field and quenching technique. Twenty seven e
nergy minima have been located at the potential energy surface of the adeni
ne thymine base pair: nine of them are H-bonded structures, eight are T-sha
ped dimers, and the remaining nine correspond to various stacked arrangemen
ts. H-bonded structures are the most stable while stacked and T-shaped stru
ctures are by more than 4 kcal/mol less stable than the global minimum, The
global minimum and the first;two local minima utilize N-9-H and N-3 groups
of adenine for the binding, i.e., the amino group N-6, and ring N-1 and N-
7 adenine positions are not involved in the base pairing. The most stable H
-bonding patterns cannot occur in nucleic acids since the Ns position is bl
ocked by the attached sugar ring. Hoogsteen and Watson-Crick type structure
s (third and fourth local minima) are by about 3 kcal/mol less stable than
the global minimum. Energetic preferences of the global minimum and first t
wo local minima were confirmed by correlated MP2 ab initio calculations wit
h 6-31G** and -6-311G(2d,p) basis sets. Relative population of various stru
ctures (a quantity proportional to Delta G of base pair formation) was dete
rmined by molecular dynamics simulations in the NVE microcanonical ensemble
. Although the stability order of the global and first two local minima is
unaffected by including the entropy contribution, the stability order of th
e remaining structures is altered rather significantly in favor of stacked
and T-shaped structures. The simulations further show that the population o
f the global minimum is about 35% and it means that experimental gas-phase
studies are likely to detect a vast number of mutually coexisting structure
s.