Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 122
and to a lesser extent by the second neighbor shell . Such a localized behavior is
expected for the quadrupole interaction since the lattice field gradient falls off
rapidly with distance ( ar - 3 ) . The fact that the isomer shift disturbance also is ...
and to a lesser extent by the second neighbor shell . Such a localized behavior is
expected for the quadrupole interaction since the lattice field gradient falls off
rapidly with distance ( ar - 3 ) . The fact that the isomer shift disturbance also is ...
Page 123
2 % at 400 K ) ( from Window , 1972b ) . charge around a central iron atom due to
the presence of iron neighbors . The distortion may be treated formally as if there
were an effective point charge on an iron neighbor in order to calculate the ...
2 % at 400 K ) ( from Window , 1972b ) . charge around a central iron atom due to
the presence of iron neighbors . The distortion may be treated formally as if there
were an effective point charge on an iron neighbor in order to calculate the ...
Page 129
6 koe is the field in fully ordered NigFe ( zero first neighbors and six second
neighbors ) and n 1 , n , the numbers of iron ... The changes in field per iron atom
in first and second nearest neighbor shells , AH , and AH 2 , were found to be
about ...
6 koe is the field in fully ordered NigFe ( zero first neighbors and six second
neighbors ) and n 1 , n , the numbers of iron ... The changes in field per iron atom
in first and second nearest neighbor shells , AH , and AH 2 , were found to be
about ...
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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