Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 95
Figures 20a and b illustrate the goodness of fit which may be obtained between
experimental and theoretical ( 111 ) intensity bands for the CuNi system using
CMS . Intermediate results after diffusing a 2 . 8 um Ni deposit for 105 min at 900°
C ...
Figures 20a and b illustrate the goodness of fit which may be obtained between
experimental and theoretical ( 111 ) intensity bands for the CuNi system using
CMS . Intermediate results after diffusing a 2 . 8 um Ni deposit for 105 min at 900°
C ...
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 ...
Page 190
Comparison between the theoretically expected behavior of the quenching ratio
Q ) , obtained from Eqs . ( 9 ) and ( 10 ) with parameters for O in GaP inserted ,
and experimentally obtained values ( + ) , for different values of the ratio 03 / 0 ...
Comparison between the theoretically expected behavior of the quenching ratio
Q ) , obtained from Eqs . ( 9 ) and ( 10 ) with parameters for O in GaP inserted ,
and experimentally obtained values ( + ) , for different values of the ratio 03 / 0 ...
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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