We have investigated the interaction of O~-with Mg 2+ ions at terraces, edges and comers and with the Fs centers of the MgO (100) surface by means of ab initio cluster model wavefunctions. While O 2 is unbound or weakly bound at surface cations, O~-is electrostatically bound with adsorption energies
Structure of Ag Clusters Grown on Fs-Defect Sites of an MgO(1 0 0) Surface
✍ Scribed by Giovanni Barcaro; Edoardo Aprà; Alessandro Fortunelli
- Publisher
- John Wiley and Sons
- Year
- 2007
- Tongue
- English
- Weight
- 683 KB
- Volume
- 13
- Category
- Article
- ISSN
- 0947-6539
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✦ Synopsis
Abstract
The structure of Ag~N~ clusters (N=1–4, 6, 8, 10), both in the gas phase and grown on the MgO(1 0 0) surface containing F~s~‐defects, has been investigated by a density functional basin‐hopping (DF‐BH) approach. In analogy with what observed in the case of gold clusters, it is found that the presence of the defect implies a double frustration and a cylindrical invariance of the metal–surface interaction, causing small Ag clusters growing around the F~s~ defect to be highly fluxional. Nevertheless, two different structural crossovers are found to be induced by the metal–defect interaction for the adsorbed clusters such that: 1) planar structures prevail for N≤4 (as in the gas phase); 2) noncrystalline (fivefold symmetric) structures, which are the lowest energy ones in the gas phase for medium sized Ag~N~ clusters (N≥7), prevail for N=6 and N=8; 3) distorted face‐centered cubic (fcc) structures grown pseudomorphically on the defected surface prevail for N=10. The transition from fivefold to fcc motifs is rationalized in terms of the double‐frustration effect, which increases the bond strain of the noncrystalline structures. Detrapping energies from the defect were also calculated; the lowest energy pathway corresponds to the detachment of a dimer.
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