Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 110
2 ) is due to the electrostatic interaction between the nuclear charge and the s
electrons . The nuclear charge radius differs for the excited and ground states ,
while the s electron charge density may be varied by changing the chemical ...
2 ) is due to the electrostatic interaction between the nuclear charge and the s
electrons . The nuclear charge radius differs for the excited and ground states ,
while the s electron charge density may be varied by changing the chemical ...
Page 174
So , e . g . , it has been demonstrated that electron excitation employing the
scanning electron microscope SEM ( in a ... High energy electrons also have an
effective excitation depth ( Murata et al . , 1971 ) , which in practice cannot easily
be ...
So , e . g . , it has been demonstrated that electron excitation employing the
scanning electron microscope SEM ( in a ... High energy electrons also have an
effective excitation depth ( Murata et al . , 1971 ) , which in practice cannot easily
be ...
Page 253
... 89 - 100 AES , see Auger electron spectroscopy Amorphous alloys , 140 - 142 ,
214 , 237 , 245246 Antiferromagnetism , 138 Atomic scattering factor , 27 Auger
electron spectroscopy , 64 , 161 , 174 Austenite , 131 - 133 , 250 retained , 22 ...
... 89 - 100 AES , see Auger electron spectroscopy Amorphous alloys , 140 - 142 ,
214 , 237 , 245246 Antiferromagnetism , 138 Atomic scattering factor , 27 Auger
electron spectroscopy , 64 , 161 , 174 Austenite , 131 - 133 , 250 retained , 22 ...
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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