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The reaction of a clean Ti (0001) surface with oxygen gas at low pressure and room temperature has been studied with low-energy electron diffraction (LEED) and Auger electron spectroscopy (AES). At low exposures (about 1 Langmuir) ap(2×2) superstructure is observed which gradually converts to 1×1 at high exposures (about 100 Langmuirs). The LEED spectra confirm that the final 1×1 structure is different from that of clean Ti (0001), while the AES spectra indicate that the final oxide is probably TiO, not TiO2. The plausibility of this indication is discussed.  相似文献   
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A LEED intensity analysis of the c(2 × 2) structure obtained upon adsorption of oxygen gas on Co {00l} is reported. Three structural models have been tested on the basis of a total of 13 LEED spectra for three angles of incidence and one azimuth. The correct model has oxygen atoms chemisorbed in the four-fold symmetrical hollows formed by four adjacent substrate atoms. Atomic arrangement and metal-oxygen distances are analogous to those found in Ni{001}c(2 × 2)O.  相似文献   
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A LEED intensity analysis of Cu{0 0 1}c(2 × 2)-Cl has given an excellent fit of theory to experiment with Cl in the fourfold symmetrical hollows in a simple overlayer structure with a Cu-Cl bond length of 2.38 Å. This structure is consistent with an analysis of angle-resolved photoemission measurements made in the same experiments and published elsewhere. These results help confirm the LEED analysis of the analogous system Ag{0 0 1}c(2 × 2)-Cl which gave the same structure, but had been rejected by an independent photoemission analysis.  相似文献   
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M. Jona 《Mikrochimica acta》1930,8(1):A49-A53
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The temperature dependence of low-energy electron diffraction (LEED) intensities has often been interpreted with kinematic theory in terms of an effective Debye temperature θDeff of the surface atoms. The validity of this procedure, often questioned in the literature, is tested with a computer experiment in which LEED spectra are calculated from dynamical theory (layer-KKR method) for a model of Ag{111} with a given value of θDeff and then the usual kinematic formulae are used to re-extract the value of θDeff. The results of the experiment indicate that this procedure yields rough values of the surface Debye temperature for electron energies higher than about 40 eV, which fluctuate substantially and tend to be somewhat smaller than that originally introduced into the model. At energies lower than about 40 eV the kinematically deduced values of θDeff are too large by 10 to 15 %.  相似文献   
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