The accuracy of atomization energies obtained from explicitly correlated co
upled-cluster R12 calculations (CC-R12)-including single and double excitat
ion operators (CCSD-R12) and a posteriori perturbative corrections for trip
le excitations [CCSD[T]-R12 and CCSD(T)-R12]-is studied for CH2((1)A(1)), N
H3, H2O, HF, N-2, CO, and F-2. The basis-set convergence with functions of
high angular momentum is demonstrated. Unlike for conventional calculations
, already the spdf saturation on nonhydrogen atoms and spd saturation on hy
drogen are sufficient for CC-R12 calculations to provide results accurate t
o within 1 kJ/mol of the limit of a complete basis. Remaining small uncerta
inties at the CCSD[T]-R12 or CCSD(T)-R12 levels are attributed to the insuf
ficient convergence within the coupled-cluster hierarchy towards the limit
of full configuration interaction. It is shown that near the basis-set limi
t (as provided by CC-R12 calculations) the CCSD[T] variant of the triples c
orrection gives, on average, results closer to the experimental data than i
ts CCSD(T) counterpart. Approximate error bars are estimated by one single
CC-R12 calculation from the difference between the CCSD[T] and CCSD(T) meth
ods and from the second-order electronic cusp correction in standard approx
imation B. (C) 2001 American Institute of Physics.