Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 29
Because there is a distribution of intensity between the central beam and the left
and right portions , the actual peak shift will be less than 8 ( A20 ) bd . It has been
shown ( Zantopulos and Jatczak , 1970 ) that the centroid of the diffracted beam ...
Because there is a distribution of intensity between the central beam and the left
and right portions , the actual peak shift will be less than 8 ( A20 ) bd . It has been
shown ( Zantopulos and Jatczak , 1970 ) that the centroid of the diffracted beam ...
Page 33
Three such procedures will be compared and then the effect of counting statistics
will be discussed . 2 . METHODS OF LOCATION OF THE DIFFRACTION PEAK
The centroid of a diffraction peak has been used in x - ray stress measurements ...
Three such procedures will be compared and then the effect of counting statistics
will be discussed . 2 . METHODS OF LOCATION OF THE DIFFRACTION PEAK
The centroid of a diffraction peak has been used in x - ray stress measurements ...
Page 160
A relatively large band tailing effect with high doping will broaden the peak and
even cause a minor shift in PL peak position with increasing doping level in the
1017 - 1018 cm - 3 range . At lower doping ( < 1016 cm - 3 ) , as sometimes ...
A relatively large band tailing effect with high doping will broaden the peak and
even cause a minor shift in PL peak position with increasing doping level in the
1017 - 1018 cm - 3 range . At lower doping ( < 1016 cm - 3 ) , as sometimes ...
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Contents
R JAMES | 2 |
Principles of XRay Stress Measurement | 4 |
Control of Accuracy and Precision | 25 |
Copyright | |
15 other sections not shown
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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