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Of Appl. , 35, 1956(1964). Wagenfeld, H, Acta Cryst. A 24, 170 (1968). , Ann. Physik (5) 36, 209 (1939). Batterman, B. W. , Acta Cryst. A 24, 150 (1968). , Hildebrandt G. , Z. Physik Dtsch. 142, 406 (1955). Wagner, H, Z. Physik Dtsch. 146, 127 (1956). Kikuta, S. , J. Phy. So. Japan 25, 924 (1968). Lefeld-Sosnowska, M. and Malgrange, C , Phys. Stat. Solidi 30, K 23 (1968). Dynamical Theory of Electron Diffraction K. Kambe and K. Moliere*) With 6 figures I. Introduction The ratio of atomic scattering cross sections for electrons and X-ray photons is given by Z-f ax 4Ucsin(#/2)) 2 f I Relativistic correction and polarization factor are neglected.
Czech. J. of Physics, B 11, 199 (1961). , Czech. J. of Physics, B 12,538 (1962). , Czech. J. of Physics, B 12, 764 (1962). , C. R. Acad. Sci. Paris, 251, 2502 (1960). , J. of Appl. Cryst. (1968), 1, 181. , Philips Research Rpts, 18, 413 (1963). , C. R. Acad. Sci. Paris, 261, 3774 (1965). , Physica Statu Solidi, 26, 469 (1968). Sommerfeld, Partial Differential equations. Academic Press, p. 52 (1949). Hattori, H. , J. Phys. Soc. Japan, 21, 1772(1966). Authier, A. and Malgrange, C, C. R. Acad. Sci.
26a), the equal intensity surfaces are hyperbolic cylinders parallel to the slit. Fringes observed on a photographic plate placed in the reflected beam will be straight lines for a plane parallel crystal (fig. 27) and hyperbolae for a wedge shaped crystal (fig. 28). Fig. 27 Spherical wave Pendellosung fringes. 8 mm thick M o K a - 1 1 1 -reflection. Fig. 28 Spherical wave Pendellosung fringes wedge shaped NaN0 3 crystal. Mo K a . 40 IV A. Authier Generalized Diffraction Theory The X-ray optics described in section II and III are related to the geometric optics in that they are ray optics.