Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 4
While not detected by mechanical methods , these stresses give rise to both a
peak shift and if they vary from point to point , line ... The third kind , which ranges
over dimensions of 1 - 1000 X , gives rise to x - ray line broadening only .
While not detected by mechanical methods , these stresses give rise to both a
peak shift and if they vary from point to point , line ... The third kind , which ranges
over dimensions of 1 - 1000 X , gives rise to x - ray line broadening only .
Page 89
Small variations in composition profile which provide large variations in slope
would be expected to give large shape changes in the band intensity . Because
the diffusion coefficient is of greater fundamental importance than the profile ...
Small variations in composition profile which provide large variations in slope
would be expected to give large shape changes in the band intensity . Because
the diffusion coefficient is of greater fundamental importance than the profile ...
Page 171
If the dopant in question causes a specific radiative emission , detection of this
emission strength will give an indication of such dopant distributions . An
example of this is shown in Fig . 11 , for epitaxial GaAs where a correlation of
growth ...
If the dopant in question causes a specific radiative emission , detection of this
emission strength will give an indication of such dopant distributions . An
example of this is shown in Fig . 11 , for epitaxial GaAs where a correlation of
growth ...
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Contents
R JAMES | 2 |
Principles of XRay Stress Measurement | 4 |
Control of Accuracy and Precision | 25 |
Copyright | |
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absorption additional allows alloy angle Appl applications atoms bandgap beam broadening cause coefficients components composition composition profile concentration constant containing cooling crystal curve defects dependent deposits depth determined developed diffraction diffusion direction discussed dislocation distance distribution effect electron elements employed energy error et al example excitation experimental factor field function give given grain heat important included increasing intensity intensity bands iron laser lattice layer less magnetic material measurements Metals method Mössbauer observed obtained occur optical parameter peak phase Phys plane position possible powder problem produce range rays recent region relative residual stress sample semiconductors shift shown single Society solid spacing specimen spectra spectrum sputtering steel structure studies substrate surface target technique temperature term thickness values variation volume x-ray