A. Nowek et J. Leszczynski, POST-HARTREE-FOCK STUDY ON AR-HCO-HCO+ COMPLEXES - A CRITICAL-EXAMINATION OF EXPERIMENTAL-DATA( AND HE), The Journal of chemical physics, 105(15), 1996, pp. 6388-6394
The second order Moller-Plesset (MP2) to the fourth order many-body pe
rturbation theory including single, double, triple, and quadruple subs
titutions (MP4(SDTQ)), coupled cluster with single and double excitati
ons (CCSD), CCSD with perturbative triple excitations [CCSD(T)], quadr
atic configuration interaction with single and double substitutions (Q
CISD), and QCISD including noniterative triples contributions [QCISD(T
)] ab initio correlated levels of theory have been employed in studies
on molecular geometry and stability of the Ar-HCO+ and He-HCO+ comple
xes. Triple-zeta split-valence (6-311G) and correlation consistent (cc
-pVTZ) basis sets augmented with diffuse and polarization functions we
re used. At applied levels of theory the predicted interaction energie
s (corrected for the basis set superposition error and zero-point vibr
ational energy) for Ar-HCO+ range from -3.21 kcal/mol (QCISD/6-311G(2d
f,2pd) to -4.21 kcal/mol (MP4(SDTQ)/aug-cc-pVTZ), and for He-HCO+ vary
from -0.12 kcal/mol (-42 cm(-1), MP2/cc-pVTZ) to -0.37 kcal/mol (-130
cm(-1), CCSD(T)/aug-cc-pVTZ//CCSD/aug-cc-pVTZ). The optimized Ar-H di
stance (2.1392 Angstrom at QCISD/cc-pVTZ and 2.1222 Angstrom at MP2/au
g-cc-pVTZ) agrees very well with the experimentally determined (2.13 A
ngstrom) value, whereas when step-by-step higher level methods and bas
is sets are applied, the predicted He-H distance (1.9156 Angstrom at Q
CISD(T)/aug-cc-pVTZ dramatically retreats from the experimental value
of 2.00 Angstrom. (C) 1996 American Institute of Physics.