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Geometric and Electronic Structure of Potassium on Rh(111)
19
Citations
19
References
1992
Year
Materials ScienceEngineeringPhysicochemical AnalysisSurface ChemistryNatural SciencesTheoretical Inorganic ChemistrySurface ScienceApplied PhysicsK-overlayer CharacterMultilayer DesorptionPhysical ChemistryQuantum ChemistryChemistryElectronic PropertiesElectronic StructureCrystallography
The interaction of potassium with Rh(111) was studied by AES, REELS, LEED, TDS, UPS and work function (WF) measurements. At low coverages (ΘK < 0.1) Φ decreases linearly followed by a shallow minimum at ΘK ≈ 0.2 and a slight reincrease. Three different LEED K-superstructures at ΘK = 0.25 (2 × 2), ΘK = 0.33 (√3 × √3 R30°) and at ΘK = 0.5 (2 × 2) have been observed corresponding to a nearest K–K neighbour distance for the first two structures of 5.38Å and 4.66Å, respectively, The √3 × √3 R30° structure is compressed by 6% compared to the surface density of (110) K planes. The multilayer desorption in TDS is observed only at K-coverages beyond 0.5 which is generally correlated with a metallic (potassium like) character of the overlayer. In the K-coverage range 0–0.33 the electronic binding energy of the K(3p) level shifts to lower binding energy (18.4–17.8 eV). Above ΘK = 0.5 a new K(3p) peak develops at the sane energetic position as it is observed for a thick potassium film (18.6 eV). The transition of the electronic properties of the K-overlayer character is also ionic (low coverage) to a covalent (high coverage) bonding character is also reflacted in the electron loss experiment. Only above ΘK = 0.5 the plasmon loss characteristic of thick metallic K at 2.5 eV can be detected, even though already around 0.33 the K–K nearest neighbour distance corresponds to the covalent value.
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