scholarly journals Holographic atomic images from surface and bulk W(110) photoelectron diffraction data

1997 ◽  
Author(s):  
P. M. Len ◽  
J. D. Denlinger ◽  
E Rotenberg ◽  
S. D. Kevan ◽  
B. P. Tonner ◽  
...  
1999 ◽  
Vol 59 (8) ◽  
pp. 5857-5870 ◽  
Author(s):  
P. M. Len ◽  
J. D. Denlinger ◽  
E. Rotenberg ◽  
S. D. Kevan ◽  
B. P. Tonner ◽  
...  

Clay Minerals ◽  
1980 ◽  
Vol 15 (3) ◽  
pp. 209-217 ◽  
Author(s):  
S. Evans ◽  
E. Raftery

AbstractX-ray photoelectron diffraction data from single crystals of a biotite containing ∼1% Ti show that although this element is located entirely in octahedral sites, the Ti sites are not precisely equivalent to those of Mg and Fe. Comparisons of Ti 2p X-ray photoelectron spectra from two biotites and from two titaniferous phlogopites (∼0·3–·5% Ti) with those from Ti(II), Ti(III) and Ti(IV) oxides indicate that this element is present as Ti(III) rather than Ti(IV) in all four micas.


Clay Minerals ◽  
1982 ◽  
Vol 17 (4) ◽  
pp. 443-452 ◽  
Author(s):  
S. Evans ◽  
E. Raftery

AbstractX-ray photoelectron diffraction data for three cleavage surfaces from a crystal of a Norwegian lepidolite containing 2·3% Rb and 3% Mn are reported and interpreted. Rubidium is shown to occupy anhydrous interlayer sites equivalent to those of potassium, and to be distributed uniformly throughout the crystals. Cleavage occurs in Mn-rich regions in which the manganese(II) is located in octahedral sites essentially equivalent to those of lithium. The octahedral Al sites can readily be distinguished from the Li,Mn sites and it is concluded that Al occupies predominantly M(2), cis sites while Li and Mn(II) prefer M(1), trans sites. Photoelectron diffraction data also indicate that 40 ± 5% of the Al is tetrahedrally coordinated, compared with a figure of ∼34% deduced independently from a surface analysis.


1993 ◽  
Vol 47 (12) ◽  
pp. 7462-7479 ◽  
Author(s):  
D. Naumović ◽  
A. Stuck ◽  
T. Greber ◽  
J. Osterwalder ◽  
L. Schlapbach

2003 ◽  
Vol 10 (06) ◽  
pp. 925-932
Author(s):  
S. H. XU ◽  
H. S. WU ◽  
S. Y. TONG ◽  
M. KEEFFE ◽  
G. J. LAPEYRE ◽  
...  

The k derivative spectra (KDS) transform is used for construction of the three-dimensional atomic structure of the C 2 H 4/ Si (100)-(2×1) system from photoelectron diffraction data. The image function obtained by the KDS transform clearly observes the second-layer Si atoms and the C emitters apart from the first-layer Si atoms. The observations of the second-layer Si atoms and the C emitters make it easy to measure the C–C bond length correctly. Then a conclusive adsorption model — the di-σ model — for the C 2 H 4/ Si (100)-(2×1) system is established. In comparison with the KDS transform, the normal small-cone transform hardly measures the C–C bond length. The ability to observe more scatterers of a photoelectron emitter by the KDS transform expands the applicability of holographic imaging.


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