Formulation of dynamical theory of X-ray diffraction for perfect crystals in the Laue case using the Riemann surface

Author:

Saka Takashi

Abstract

The dynamical theory for perfect crystals in the Laue case was reformulated using the Riemann surface, as used in complex analysis. In the two-beam approximation, each branch of the dispersion surface is specified by one sheet of the Riemann surface. The characteristic features of the dispersion surface are analytically revealed using four parameters, which are the real and imaginary parts of two quantities specifying the degree of departure from the exact Bragg condition and the reflection strength. By representing these parameters on complex planes, these characteristics can be graphically depicted on the Riemann surface. In the conventional case, the absorption is small and the real part of the reflection strength is large, so the formulation is the same as the traditional analysis. However, when the real part of the reflection strength is small or zero, the two branches of the dispersion surface cross, and the dispersion relationship becomes similar to that of the Bragg case. This is because the geometrical relationships among the parameters are similar in both cases. The present analytical method is generally applicable, irrespective of the magnitudes of the parameters. Furthermore, the present method analytically revealed many characteristic features of the dispersion surface and will be quite instructive for further numerical calculations of rocking curves.

Publisher

International Union of Crystallography (IUCr)

Subject

Inorganic Chemistry,Physical and Theoretical Chemistry,Condensed Matter Physics,General Materials Science,Biochemistry,Structural Biology

Reference19 articles.

1. Abramowitz, M. & Stegun, I. A. (1965). Handbooks of Mathematical Functions with Formulas, Graphs, and Mathematical Tables, p. 17. New York: Dover.

2. Authier, A. (2001). Dynamical Theory of X-ray Diffraction. New York: Oxford University Press.

3. Dynamical Diffraction of X Rays by Perfect Crystals

4. X-ray diffraction when the real part of the scattering factor is zero

5. Dynamical diffraction in the Laue case with Borrmann absorption

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