EXPLICITLY CORRELATED COUPLED-CLUSTER CALCULATIONS OF THE DISSOCIATION-ENERGIES AND BARRIERS TO CONCERTED HYDROGEN-EXCHANGE OF (HF)(N) OLIGOMERS (N = 2, 3, 4, 5)
W. Klopper et al., EXPLICITLY CORRELATED COUPLED-CLUSTER CALCULATIONS OF THE DISSOCIATION-ENERGIES AND BARRIERS TO CONCERTED HYDROGEN-EXCHANGE OF (HF)(N) OLIGOMERS (N = 2, 3, 4, 5), Molecular physics, 94(1), 1998, pp. 105-119
The electronic dissociation energies and barriers to concerted hydroge
n exchange of (HF), oligomers with n = 2,...,5 are computed by means o
f a many-body decomposition of the total electronic energy. The one-an
d two-body terms are obtained from explicitly correlated coupled clust
er calculations including singles, doubles, and a perturbative triples
correction (CCSD(T)-R12), in a large Gaussian basis set consisting of
276 contracted atomic functions. The three-body term is computed at t
he conventional CCSD(T) level in a basis set containing 228 functions.
The four-and five-body terms are obtained from explicitly correlated
second-order perturbation theory calculations (MP2-R12), using basis s
ets with 305 (tetramer) and 380 (pentamer) functions. Since the many-b
ody terms are computed using the same basis set (i.e. the basis of the
largest fragment) for all fragments and subfragments, our calculation
s implicitly include a counterpoise correction. The results of the cal
culations are compared with semi-empirical one-, two-, and three-body
potentials, and new best estimates of the electronic dissociation ener
gies and barriers are inferred. For (HF)(2), (HF)(3), (HF)(4), and (HF
)(5), respectively, we obtain for the electronic dissociation energies
into monomers 19.1(2), 64(2), 116(3) and 158(4)kJ mol(-1), and for th
e electronic barriers to concerted hydrogen exchange 175(10), 85(10),
60(10) and 65(10) kJ mol(-1). The results are shown to be consistent w
ith NMR line broadening data within the framework of transition state
theory.