The results of a systematic study of the interaction of small coinage metal clusters (Mn, n=1-3) and extended deposition (1 ML and 2 ML) with the regular and locally defected (Fs center and divacancy) neutral MgO (100) surface are presented. The calculations have been performed at the DFT level employing Plane Waves as basis set and using a gradient-corrected exchange-correlation functional (PW91). The adhesion energy along the group follow a trend which can be rationalized in terms of the strength and stickiness of the metallic bond, electrostatic polarization effects and chemical interactions. Coinage metal dimers and trimers are absorbed on the regular surface in an up-right position with little modifications with respect to the gas-phase structure, and can easily diffuse from site to site (in the case of trimers, also because of their fluxional character). In the case of extended deposition, the adhesion energy increases when passing from 1 ML to 2 ML due to a metal-on-top stabilization mechanism. Neutral localized defects on the surface such as the Fs center (generated by a missing O atom) and the double vacancy (generated by a missing MgO dimer) act as strong trapping centers for small clusters and remarkably increase the adhesion of metal slabs to the surface in the case of extended deposition. At variance with the Fs center, the double vacancy induces a strong structural and energetical modification of the surrounding oxide lattice, varying also as a function of the metal deposition. A peculiar structural rearrangement consisting in the segregation of the metal slab into islands on the surface is observed in the case of 1ML Cu and (to a lesser extent) Au.
The interaction of coinage metal clusters with the MgO(100) surface
Barcaro G;Fortunelli A
2005
Abstract
The results of a systematic study of the interaction of small coinage metal clusters (Mn, n=1-3) and extended deposition (1 ML and 2 ML) with the regular and locally defected (Fs center and divacancy) neutral MgO (100) surface are presented. The calculations have been performed at the DFT level employing Plane Waves as basis set and using a gradient-corrected exchange-correlation functional (PW91). The adhesion energy along the group follow a trend which can be rationalized in terms of the strength and stickiness of the metallic bond, electrostatic polarization effects and chemical interactions. Coinage metal dimers and trimers are absorbed on the regular surface in an up-right position with little modifications with respect to the gas-phase structure, and can easily diffuse from site to site (in the case of trimers, also because of their fluxional character). In the case of extended deposition, the adhesion energy increases when passing from 1 ML to 2 ML due to a metal-on-top stabilization mechanism. Neutral localized defects on the surface such as the Fs center (generated by a missing O atom) and the double vacancy (generated by a missing MgO dimer) act as strong trapping centers for small clusters and remarkably increase the adhesion of metal slabs to the surface in the case of extended deposition. At variance with the Fs center, the double vacancy induces a strong structural and energetical modification of the surrounding oxide lattice, varying also as a function of the metal deposition. A peculiar structural rearrangement consisting in the segregation of the metal slab into islands on the surface is observed in the case of 1ML Cu and (to a lesser extent) Au.File | Dimensione | Formato | |
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