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- W2032252439 abstract "The scattering of electrons by stacking faults is formulated for both h.c.p. and f.c.c. structures using orthogonalized-plane-waves and time dependent perturbation theory. For highenergy electrons (several times the Fermi energy) ordinary diffraction is obtained, with transition amplitudes first-order in the lattice potential. This scattering is not specular. At lower energies, corresponding to the Fermi energy in polyvalent metals, only electrons with large angles of incidence are diffracted to this order. Electrons with small angles of incidence are scattered only to higher order in the potential and only into the specularly reflected state. At still lower energies, corresponding to the Fermi energy in monovalent metals, all electrons are subject only to higher-order specular scattering. Stacking faults in zinc are treated in detail. The calculation of the second-order transition rate for normally incident electrons shows that it is more important to take into account the interaction of the band structure with the defect scattering than to go to second order in the scattering by the defect potential alone. This latter contribution may be written in terms of residues at complex wave-numbers corresponding to Tamm waves originating at the stacking fault. Cross sections are obtained for several incident directions to illustrate first-order non-specular transitions, second-order specular transitions, and the scattering of band states at the zone faces." @default.
- W2032252439 created "2016-06-24" @default.
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- W2032252439 date "1965-03-01" @default.
- W2032252439 modified "2023-09-27" @default.
- W2032252439 title "Scattering from planar defects in metals" @default.
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- W2032252439 doi "https://doi.org/10.1016/0022-3697(65)90121-6" @default.
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