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Propagation of X-ray beams in distorted crystals (Bragg case). I. The case of weak deformations

Propagation of X-ray beams in distorted crystals (Bragg case). I. The case of weak deformations It has been commonly admitted that the theories of X-ray propagation in distorted crystals based on the principles of geometrical optics Penning & Polder (1961). Philips Res. Rep. 16, 419-440; Kato (1963). J. Phys. Soc. Jpn, 18, 1785-1791; Kato (1964). J. Phys. Soc. Jpn, 19, 67-71, 971-985 were applicable only in the transmission (Laue) case. It is demonstrated in this paper that they can be applied more generally in all cases where beams can be defined, i.e. also in the Bragg case outside the total reflection range. Simple formulae for the case of a constant strain gradient in symmetric Bragg geometry are derived from a general formulation of the basic equation of geometrical theory using a new universal parameter a. They are verified by solving Takagi's equations numerically. The results are visualized by means of an original method of ray tracing directly from Takagi's equations. http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.png Acta Crystallographica Section A: Foundations of Crystallography International Union of Crystallography

Propagation of X-ray beams in distorted crystals (Bragg case). I. The case of weak deformations

Propagation of X-ray beams in distorted crystals (Bragg case). I. The case of weak deformations


Abstract

It has been commonly admitted that the theories of X-ray propagation in distorted crystals based on the principles of geometrical optics Penning & Polder (1961). Philips Res. Rep. 16, 419-440; Kato (1963). J. Phys. Soc. Jpn, 18, 1785-1791; Kato (1964). J. Phys. Soc. Jpn, 19, 67-71, 971-985 were applicable only in the transmission (Laue) case. It is demonstrated in this paper that they can be applied more generally in all cases where beams can be defined, i.e. also in the Bragg case outside the total reflection range. Simple formulae for the case of a constant strain gradient in symmetric Bragg geometry are derived from a general formulation of the basic equation of geometrical theory using a new universal parameter a. They are verified by solving Takagi's equations numerically. The results are visualized by means of an original method of ray tracing directly from Takagi's equations.

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Publisher
International Union of Crystallography
Copyright
Copyright (c) 1984 International Union of Crystallography
ISSN
0108-7673
DOI
10.1107/S0108767384001082
Publisher site
See Article on Publisher Site

Abstract

It has been commonly admitted that the theories of X-ray propagation in distorted crystals based on the principles of geometrical optics Penning & Polder (1961). Philips Res. Rep. 16, 419-440; Kato (1963). J. Phys. Soc. Jpn, 18, 1785-1791; Kato (1964). J. Phys. Soc. Jpn, 19, 67-71, 971-985 were applicable only in the transmission (Laue) case. It is demonstrated in this paper that they can be applied more generally in all cases where beams can be defined, i.e. also in the Bragg case outside the total reflection range. Simple formulae for the case of a constant strain gradient in symmetric Bragg geometry are derived from a general formulation of the basic equation of geometrical theory using a new universal parameter a. They are verified by solving Takagi's equations numerically. The results are visualized by means of an original method of ray tracing directly from Takagi's equations.

Journal

Acta Crystallographica Section A: Foundations of CrystallographyInternational Union of Crystallography

Published: Sep 1, 1984

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