Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 33
020 ) a Ten measurements with a PSD , many points in the profile . FWHM is the
full - width at half of the maximum intensity . c Air cooled from 820° C , then stress
relieved by slow cooling from 677° C to produce a sharp profile . d The term in ...
020 ) a Ten measurements with a PSD , many points in the profile . FWHM is the
full - width at half of the maximum intensity . c Air cooled from 820° C , then stress
relieved by slow cooling from 677° C to produce a sharp profile . d The term in ...
Page 124
produced by arc melting and cold rolling , has the same singlet and doublet
structure ( Fig . 8 ) as observed for dilute Au Fe alloys , but here the relative area
of the doublet is anomalously large ( 55 % total area ) due to pronounced iron -
iron ...
produced by arc melting and cold rolling , has the same singlet and doublet
structure ( Fig . 8 ) as observed for dilute Au Fe alloys , but here the relative area
of the doublet is anomalously large ( 55 % total area ) due to pronounced iron -
iron ...
Page 126
Thus , as well as being able to produce higher iron concentrations by
implantation , one may also study the effects on the spectra of the defects
produced by the radiation damage during implantation . In fact , because of
sputtering of target ...
Thus , as well as being able to produce higher iron concentrations by
implantation , one may also study the effects on the spectra of the defects
produced by the radiation damage during implantation . In fact , because of
sputtering of target ...
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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