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Tuning the surface metal work function by deposition of ultrathin oxide films: Density functional calculations
255
Citations
36
References
2006
Year
EngineeringCharge TransferThin Film Process TechnologyMetal Electron DensitySurface DipoleThin Film ProcessingMaterials ScienceNanotechnologyUltrathin Oxide FilmsOxide ElectronicsSurface CharacterizationMaterial AnalysisSurface ScienceApplied PhysicsCondensed Matter PhysicsSurface EngineeringThin FilmsDensity Functional CalculationsSurface Processing
Changes in the work function $\ensuremath{\Phi}$ of metal surfaces upon deposition of ultrathin oxide films have been studied by means of band structure density functional theory calculations. Four systems have been considered: $\mathrm{MgO}∕\mathrm{Ag}(100)$, $\mathrm{MgO}∕\mathrm{Mo}(100)$, ${\mathrm{TiO}}_{2}∕\mathrm{Mo}(100)$, and ${\mathrm{SiO}}_{2}∕\mathrm{Mo}(112)$. $\mathrm{MgO}$ films induce a decrease of $\ensuremath{\Phi}$ of 1 to $2\phantom{\rule{0.3em}{0ex}}\mathrm{eV}$ compared to the clean metal substrate; ${\mathrm{SiO}}_{2}$ and ${\mathrm{TiO}}_{2}$ induce an increase of $\ensuremath{\Phi}$ of about $0.5--1\phantom{\rule{0.3em}{0ex}}\mathrm{eV}$. The reasons for this behavior are different: for ${\mathrm{TiO}}_{2}$ and ${\mathrm{SiO}}_{2}$ the work function increase can be explained with the classical model of surface dipole due to metal-to-oxide charge transfer at the interface. On $\mathrm{MgO}∕\mathrm{metal}$ interfaces, where the charge transfer is negligible, the shift is due to the compression of the metal electron density enforced by the oxide layer, with consequent change in surface dipole. The results suggest that by appropriately choosing the metal support and the oxide film one can design nanostructured materials with new properties.
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