Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 112
where e is the electronic charge , Q the nuclear quadrupole moment , and m ; = 1
, 1 – 1 , · · · , I the nuclear magnetic spin quantum number . The electric field
gradient tensor may be specified by two components , Vez = a2VlaZo being the ...
where e is the electronic charge , Q the nuclear quadrupole moment , and m ; = 1
, 1 – 1 , · · · , I the nuclear magnetic spin quantum number . The electric field
gradient tensor may be specified by two components , Vez = a2VlaZo being the ...
Page 127
Aging of the sample allows the a - iron precipitates to grow sufficiently to produce
the six line magnetic spectrum of bulk a iron . B . Magnetic Alloys The spectra for
magnetic alloys of for example FeX may be analyzed similarly into magnetic ...
Aging of the sample allows the a - iron precipitates to grow sufficiently to produce
the six line magnetic spectrum of bulk a iron . B . Magnetic Alloys The spectra for
magnetic alloys of for example FeX may be analyzed similarly into magnetic ...
Page 140
It is this locking of the spin directions which gives rise to magnetic splitting in the
Mössbauer spectra for less than – 10 % iron and also to the sharp maximum in
the low field magnetic susceptibility ( Cannella et al . , 1971 ) . This also explains
...
It is this locking of the spin directions which gives rise to magnetic splitting in the
Mössbauer spectra for less than – 10 % iron and also to the sharp maximum in
the low field magnetic susceptibility ( Cannella et al . , 1971 ) . This also explains
...
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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