There is an unresolved discrepancy between theory and experiment about the observed hindrance in dissociative adsorption of O2 on Al(111). In an attempt to understand the hindrance, we have investigated the interaction of O2 with a tetrahedral Al4 cluster (the apex considered as adatom) in a total singlet state by employing both the multireference configuration interaction (MRCI) and the density functional theory (DFT) methods. For an approach of O2 facing an apex of the Al4 pyramid and parallel to its base, both the MRCI and the DFT calculations show that after an early barrier the system goes through a narrow local minimum before it reaches a deep minimum of ∼203 kcal/mol near the pyramid base. The O2 molecule opens continuously, followed by a small decrease in the O–O distance around the deep minimum, forming antibonding orbitals with the pyramid base, whereas the O–O distance starts increasing in further increasing the incident energy. These results differ from previous results obtained for the same system but in a total triplet state, which showed two similar minima (one local narrow and one deep) but where O2 is dissociatively adsorbed to the pyramid base, forming bonding orbitals with it. The reason for this difference is discussed. Total triplet is an excited state where the bound O–O becomes spinless and the spin density is transferred to the pyramid apex. Similar transfers occur on an Al16 cluster formed by extending the pyramid base to a (111) arrangement. Our findings are contrasted with known results about the interaction of O2 with Si clusters. The effect of the spin state on the interaction of O2 with the planar Al base suggests that spin should be considered in an analysis of O2 adsorption on aluminum surfaces as well. To our understanding, to increase the sticking probability, free O2 must be, before incidence, prepared in singlet.
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