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Scats backs

The periodicity of this modulation of the absorption will be dependent upon the inteiatomic distance between the absorbing and back-scat tei i ng atoms, R, and the phase shifts, 5. , encountered when the photoelect i on expeiiences the potentials at these centres. Its intensity will be governed by the number of back-scatterers, Nj and their back-scattering amplitudes, F (k). Finally the amplitude is dampened by disorder (thermal and static), a in the interatomic distance and any inelastic piocesses (related to the mean free path of the election, j)- The recognition of the stiuctural information intrinsic to this phenomenon and the derivation of a tractable formula for the estimation of interatomic distances was the result of the work of Sayers, Lytle and... [Pg.7]

Fig. I. Back scatting image of the ZrC/Ti3AIC2 composite, showing an uniform distribution of ZrC particles (gray phase) in Ti3AIC2 matrix containing smdl amount of AI2O3 particles (dark phase). Fig. I. Back scatting image of the ZrC/Ti3AIC2 composite, showing an uniform distribution of ZrC particles (gray phase) in Ti3AIC2 matrix containing smdl amount of AI2O3 particles (dark phase).

See other pages where Scats backs is mentioned: [Pg.196]    [Pg.128]    [Pg.238]    [Pg.145]    [Pg.128]    [Pg.411]    [Pg.745]   
See also in sourсe #XX -- [ Pg.30 , Pg.32 , Pg.78 ]




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