Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 72
Likewise , the ß phase may be located well below the free surface , and because
of absorption , the effective volume could be zero . The effective volume
measured by reflection geometry must therefore include appropriate absorption
and ...
Likewise , the ß phase may be located well below the free surface , and because
of absorption , the effective volume could be zero . The effective volume
measured by reflection geometry must therefore include appropriate absorption
and ...
Page 109
A similar f factor determines the probability for resonant absorption . Thus for a
non - negligible value of f , the nucleus or atom should be tightly bound in a solid
and the y - ray energy should be low ( in practice Ž 100 keV ) . In addition ...
A similar f factor determines the probability for resonant absorption . Thus for a
non - negligible value of f , the nucleus or atom should be tightly bound in a solid
and the y - ray energy should be low ( in practice Ž 100 keV ) . In addition ...
Page 179
This has been a traditional technique for obtaining optical information about
defect absorption ( Klick and Schulman , 1957 ) , as well as fundamental
absorption of a material ( Dean , 1968 ; Monemar , 1973 , 1974 ) . Many recent
applications ...
This has been a traditional technique for obtaining optical information about
defect absorption ( Klick and Schulman , 1957 ) , as well as fundamental
absorption of a material ( Dean , 1968 ; Monemar , 1973 , 1974 ) . Many recent
applications ...
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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