Abstract
A computing method for the forward dynamical scattering calculations which has been successfully applied to the Bragg case of high energy electron diffraction is described. This method is based on the physical optics theory of dynamical diffraction of Cowley and Moodie and is used for calculations of reflection high energy electron diffraction (RHEED) diffraction amplitudes and the reflection electron microscopy (REM) image intensities for the extended surface of a perfect crystal and also for a crystal surface with a defect. The physical basis of the method and some practical computing considerations are described.
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