Abstract:Unoccupied density of states (DOS) for the polar (0001) Zn, (000 1) O and non-polar (10 10) ZnO surfaces and for a MgO(001)-c(2 × 2) thin film were studied using total current spectroscopy (TCS). TC spectra of the ZnO surfaces reveal the Zn 4s-O 2p band (6.2 eV) and two DOS maxima in the Zn 4p-O 2p band which exhibited different energy positions on the Zn-terminated (8.1 eV) and O-terminated (11.0 eV) surfaces. In the TC spectra of the MgO thin film, the energy location of Mg-derived (8.0, 14.8 and 21.0 eV) an… Show more
“…The clean surface thus prepared gave a sharp (1×1) LEED pattern. The work function of the clean surface was typically 4.5-4.9 eV, in good agreement with the literature values of 4.64-5.05 eV [10][11][12].…”
The geometric and electronic properties of alkali metals (Na and Cs) on ZnO(1010) are investigated by means of photoelectron spectroscopy and low energy electron diffraction (LEED). Growth of the Na overlayer on ZnO(1010) at room temperature is characterized by layer-by-layer growth or monolayer growth followed by three-dimensional cluster growth. The Na adatoms in the first layer are in a cationic state, and the metallic phase is formed on top of the first cationic layer. Although Na deposition at room temperature does not yield any long-range ordered superstructure, annealing the Na-covered surface results in a (1×3) LEED pattern, and we propose the formation of the Na atomic chains along the Zn-O dimer rows. For the Cs adsorption system, the disordered overlayer by ionized Cs adatoms is also formed throughout the submonolayer coverage region. Unlike the Na adsorption system, heat treatment of the Cs-covered surface does not yield any ordered structure until all Cs adatoms desorb from the surface.
“…The clean surface thus prepared gave a sharp (1×1) LEED pattern. The work function of the clean surface was typically 4.5-4.9 eV, in good agreement with the literature values of 4.64-5.05 eV [10][11][12].…”
The geometric and electronic properties of alkali metals (Na and Cs) on ZnO(1010) are investigated by means of photoelectron spectroscopy and low energy electron diffraction (LEED). Growth of the Na overlayer on ZnO(1010) at room temperature is characterized by layer-by-layer growth or monolayer growth followed by three-dimensional cluster growth. The Na adatoms in the first layer are in a cationic state, and the metallic phase is formed on top of the first cationic layer. Although Na deposition at room temperature does not yield any long-range ordered superstructure, annealing the Na-covered surface results in a (1×3) LEED pattern, and we propose the formation of the Na atomic chains along the Zn-O dimer rows. For the Cs adsorption system, the disordered overlayer by ionized Cs adatoms is also formed throughout the submonolayer coverage region. Unlike the Na adsorption system, heat treatment of the Cs-covered surface does not yield any ordered structure until all Cs adatoms desorb from the surface.
“…Moreover, feature A is more peaked in the TEYN spectra indicating that it is more sensitive to surface states. Feature A has been proposed to be associated to σ-type interaction between Zn and O planes27. Modification of its intensity and energy can be related to surface relaxation phenomena.…”
Section: Resultsmentioning
confidence: 99%
“…In contrast, the spectra corresponding to the film of lowest thickness exhibit increased and decreased intensity of the B and A contribution with reference to the thickest films, respectively. The high amplitude of feature B indicates the surface is (0001) O-terminated2728. The much weaker amplitude of feature A indicates a lower hybridization of Zn and O atoms.…”
The excitonic light emission of ZnO films have been investigated by means of photoluminescence measurements in ultraviolet-visible region. Exciton confinement effects have been observed in thin ZnO coatings with thickness below 20 nm. This is enhanced by a rise of the intensity and a blue shift of the photoluminescence peak after extraction of the adsorbed species upon annealing in air. It is found experimentally that the free exciton energy (determined by the photoluminescence peak) is inversely proportional to the square of the thickness while core-level binding energy is inversely proportional to the thickness. These findings correlate very well with the theory of kinetic and potential confinements.
“…The latter is even more pronounced for ZnO. 43,44 Following the dipole-transition selection rule, 45 the features in the O K-edge spectra (Fig. 12(a)) are excitations related from O 1s to Fig.…”
Section: Investigation Of the Electronic Properties Of Fluorine Treatmentioning
The structure, electronic properties, and surface acidity of polycrystalline ZnO are modified using F2(g). The amount of F incorporated influences the samples' properties, which were studied using, e.g., FT-IR, XPS, TEM, NMR, and microcalorimetry.
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