Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 66
This assumes that the sample is a random powder and this is seldom realized for
solid samples subjected to high temperatures . Two M . S . Theses were carried
out using 2 . 5 um of Ni electroplated onto a thick polycrystalline Cu substrate ...
This assumes that the sample is a random powder and this is seldom realized for
solid samples subjected to high temperatures . Two M . S . Theses were carried
out using 2 . 5 um of Ni electroplated onto a thick polycrystalline Cu substrate ...
Page 122
The intensity of each subspectrum is a function of concentration c of B atoms and
for a random alloy is given by 12 ! P ( n ) = ( 7 ) ( 12 - ni ni c ( 1 - c ) 12 - n where n
is the number of nearest neighbor B atoms . Although the crystal symmetry ...
The intensity of each subspectrum is a function of concentration c of B atoms and
for a random alloy is given by 12 ! P ( n ) = ( 7 ) ( 12 - ni ni c ( 1 - c ) 12 - n where n
is the number of nearest neighbor B atoms . Although the crystal symmetry ...
Page 140
spin directions “ freeze out ” cooperatively , that is they become locked in random
directions with no overall long range order . It is this locking of the spin directions
which gives rise to magnetic splitting in the Mössbauer spectra for less than ...
spin directions “ freeze out ” cooperatively , that is they become locked in random
directions with no overall long range order . It is this locking of the spin directions
which gives rise to magnetic splitting in the Mössbauer spectra for less than ...
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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