Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 218
ASESO SO 2 3 68 2 2 3 $ 100 um Fig . 2 . Microstructure of a compacted powder
target composite of 50 at . % Ni ( dark phase ) and 50 at . % Ag ( light phase ) .
ing and sintering . If the powders are not bonded. 218 S . D . DAHLGREN.
ASESO SO 2 3 68 2 2 3 $ 100 um Fig . 2 . Microstructure of a compacted powder
target composite of 50 at . % Ni ( dark phase ) and 50 at . % Ag ( light phase ) .
ing and sintering . If the powders are not bonded. 218 S . D . DAHLGREN.
Page 219
Ribbons can be rolled to 50 um thickness , which is about the size of the powders
used in the compacted powder targets . ... As with powder targets , ribbon targets
were consolidated by high - rate compaction , but a cross - rolling technique ...
Ribbons can be rolled to 50 um thickness , which is about the size of the powders
used in the compacted powder targets . ... As with powder targets , ribbon targets
were consolidated by high - rate compaction , but a cross - rolling technique ...
Page 229
Arc melted buttons , solid ductile targets and target supports for bonded
compacted powders or ribbons often were electron - beam welded directly to a
water - cooling jacket . This was a very effective approach for target preparation ...
Arc melted buttons , solid ductile targets and target supports for bonded
compacted powders or ribbons often were electron - beam welded directly to a
water - cooling jacket . This was a very effective approach for target preparation ...
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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