Improved calculations of Bragg peak intensities near atomic resonance are obtained by including the effect of the local environment around the resonant atoms on the resonant scattering amplitudes Δf=f^'+if^''. Theoretical absorption cross sections calculated by the ab initio x-ray-absorption code FEFF are used to obtain the imaginary part f^'' by extension of the optical theorem to nonforward scattering under the dipole approximation. The real part f^' is obtained by a limited range Kramers-Kronig transform of the difference between f^'' based on FEFF and existing theoretical calculations of f^'' based on an isolated-atom model. The atomic part of Δf calculated by FEFF for the resonant atom embedded in the local potential is assumed to have spherical symmetry; however, no restriction is placed on the spectral features due to multiple scattering of the intermediate-state virtual photoelectron. Bragg peak intensities calculated in the kinematic approximation using the FEFF-based Δf are compared to intensities calculated using the isolated-atom Δf and to experimental data for Cu metal and YBa₂Cu₃O6.8 at the Cu K absorption edge, and for UO₂ at the U MIV absorption edge.
No takes yet. Share an insight, caveat, or question.
Cross et al. (1998) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: