Precision Determination of Lattice Constants with a Geiger-Counter X-Ray Diffractometer

1955 ◽  
Vol 99 (6) ◽  
pp. 1737-1743 ◽  
Author(s):  
A. Smakula ◽  
J. Kalnajs
1967 ◽  
Vol 22 (1) ◽  
pp. 92-95 ◽  
Author(s):  
W. Witt

An absolute precision determination of lattice constants by electron diffraction is made with thin monocrystalline films of germanium and aluminium, having a thickness between 1000 and 5000 A. The films are prepared from the bulk material by mechanical polishing and subsequent chemical polishing or etching. The obtained values for the lattice constant α of both materials are within the accuracy Δα/α= ±3·10-5 of measurement in full agreement with the corresponding values obtained by X-ray diffraction (Smakula and Kalnajs).


1979 ◽  
Vol 34 (8) ◽  
pp. 1165-1166 ◽  
Author(s):  
Gunter Steinberg ◽  
Hans-Uwe Schuster

The X-ray structure determination of YLiSn showed that Li and Sn form a weakly distorted Wurtzit-type lattice, whose octahedral lacunas are occupied by Y. The lattice constants of the hoxagonally crystallizing compound are a = 929.6 pm and c = 734.6 pm, space group P 63mc, Z = 8


1957 ◽  
Vol 1 ◽  
pp. 131-142
Author(s):  
Otto Renius

AbstractWork at the Detroit Arsenal has shown that techniques similar to those employed for the determination of pole figures of metals can be utilized for studying organic materials such a a stretched rubber latex. The rubber, when stretched, forms a preferred orientation pattern which is proportional in intensity to the degree of elongation, and which can be used to plot a pole figure.A Geiger-counter spectrometer was used to study samples of rubber stretched 600 to 1000 per cent. Using a transmission technique, the specimens were tilted to the impinging X-ray beam in five degree increments while rotating through 360 degrees to allow the measurement of the diffracted beam from the selected atomic planes at various angles within the specimen. The intensities of the diffracted beam at these angles were plotted on a stereographic net to form the pole figures of the (002) and (012) planes of the stretched rubber. The geometry of the sample arrangements permitted the outer portion of the pole figure to be plotted from alpha angle 0 degrees to alpha angle 45 degrees.


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