EXPLICITLY CORRELATED COUPLED-CLUSTER CALCULATIONS OF THE DISSOCIATION-ENERGIES AND BARRIERS TO CONCERTED HYDROGEN-EXCHANGE OF (HF)(N) OLIGOMERS (N = 2, 3, 4, 5)

Citation
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
Citations number
69
Categorie Soggetti
Physics, Atomic, Molecular & Chemical
Journal title
ISSN journal
00268976
Volume
94
Issue
1
Year of publication
1998
Pages
105 - 119
Database
ISI
SICI code
0026-8976(1998)94:1<105:ECCCOT>2.0.ZU;2-A
Abstract
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.