Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
From inside the book
Results 1-3 of 19
Page 80
Figure 7 illustrates how the path length within a sample changes with the order of
the intensity band . It is this change that allows ( w ) ... ( 1 ) Obtain rocking curve
data on at least two intensity bands , for two orders . If the axial divergence is
large ...
Figure 7 illustrates how the path length within a sample changes with the order of
the intensity band . It is this change that allows ( w ) ... ( 1 ) Obtain rocking curve
data on at least two intensity bands , for two orders . If the axial divergence is
large ...
Page 89
intensity is spread over a large 20 range ( see Cu - Au in Table II ) , a larger
fraction of TDS will be included . One can estimate the importance of this
contribution to the intensity band by using existing corrections over the full 20
range of a band ...
intensity is spread over a large 20 range ( see Cu - Au in Table II ) , a larger
fraction of TDS will be included . One can estimate the importance of this
contribution to the intensity band by using existing corrections over the full 20
range of a band ...
Page 91
Computer simulated Moka , ( 333 ) x - ray intensity bands corresponding to the
profiles given in Fig . 12 . A Gaussian broadening function with a 0 . 13o halfwidth
is used for the entire band . The g factor is unity and lattice parameter data for the
...
Computer simulated Moka , ( 333 ) x - ray intensity bands corresponding to the
profiles given in Fig . 12 . A Gaussian broadening function with a 0 . 13o halfwidth
is used for the entire band . The g factor is unity and lattice parameter data for the
...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
R JAMES | 2 |
Principles of XRay Stress Measurement | 4 |
Control of Accuracy and Precision | 25 |
Copyright | |
15 other sections not shown
Other editions - View all
Common terms and phrases
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