Abstract: | The 6-31G ++ basis set is described. This basis set is very similar to the existing 6-31G ** set but is somewhat smaller through the use of five (rather than six) second-order Gaussians (d functions) and has polarization function exponents optimized for correlated rather than Hartree–Fock wavefunctions. The performance of 6-31G ++ is compared with that of the 6-31G ** and 6-31G ** basis sets through calculation of the geometries and atomization energies for the set of molecules LiH, FH, H2O, NH3, CH4, N2, CO, HCN, and HCCH. |