(2) ind based on KS orbitals and the infinite-order induction correction that is contained in δE HF , which subtracts out second-order corrections based on HF theory [Eq. (10)]. This is done to avoid contaminating E ind with other energy components that are present in a supramolecular KS-DFT calculation. While SAPT0(LRC-ω GDD PBE)/jun-cc-pVDZ errors are perhaps acceptable, dispersion-dominated outliers are larger when the aug-cc-pVTZ basis set is used; see Fig. ). For second-order SAPT0 calculations, there seems to be no reason to recommend using a SCF method other than HF theory. That is especially true when XC functionals lacking correct asymptotic behavior are inserted into the SAPT0 formalism, as demonstrated by results using BLYP and B3LYP in Fig. .