While the attempts currently in progress in several groups for the rigorous
inclusion of dispersion interactions in density functional theory (DFT) ca
lculations mature and evolve into practical methodology, we contribute to t
he debate on the applicability of current functionals to the calculation of
weak interaction with a systematic investigation of a few, typical, weakly
bound systems. We have used both pure DFT and a hybrid approach in which t
he total interaction energy is partitioned into two parts: (a) the dispersi
on energy which, in a first approximation is the contribution due to interm
onomer correlations and (b) all other interactions. The first component is
accurately obtained at all distances of interest by means of a well-known d
amped multipolar expansion of the dispersion energy while for the second co
mponent different approximations will be evaluated. The need to avoid doubl
e counting a fraction of the correlation energy when using the hybrid appro
ach and the choice of the appropriate functional are also discussed. We con
sider four systems of increasing binding strength, namely the Ar-2 and Kr-2
dimers, the benzene dimer, the water dimer, and a few metal carbonyls. For
pure DFT calculations we confirm the conclusion reached by others concerni
ng (a) the strong dependence of the results on the choice of the GGA functi
onal for dispersion-dominated interaction (noble gases and benzene) with th
e overall tendency to yield underbinding and (b) the relatively accurate, f
unctional-independent, description for that DFT gives of water, which we at
tribute to the fact that this system is dominated by electrostatic interact
ions. For the carbonyls we find that DFT yields results which area again st
rongly dependent on the choice of the functional and show a tendency to giv
e overbinding. Our hybrid method shows instead shortcomings only for the no
ble gases. The problem in this case is traceable to the well-known difficul
ties that all current functionals experience at medium-large intermonomer s
eparations. The quality of the hybrid results improves markedly for benzene
due to the large value of both dispersion and repulsive interactions at th
e equilibrium distance for this dimer, which makes the balance between the
two, less delicate. Excellent results are also obtained for water (for the
same reason as indicated above) and more significantly for the carbonyls wh
ere we find that dispersion contributes to the binding more than it could b
e guessed a priori. We do not claim to have found a general solution to thi
s difficult problem, but we aim at providing a quantitative assessment to w
here the problems are pointing at directions from which a general solution
may, eventually, emerge. (C) 2001 American Institute of Physics.