Dynamical theory of diffraction: Difference between revisions

Revision as of 20:48, 10 August 2006

Revision as of 20:35, 29 August 2006

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[[Image:LaueBraggGeometry.png|thumb|right|250px|Laue and Bragg geometries, top and bottom, as distinguished by the [[:en:Dynamical theory of diffraction|Dynamical theory of diffraction]] with the Bragg diffracted beam leaving the back or front surface of the crystal, respectively. ([http://www.kdliss.de/KDL/DissLiss/index.html Ref.])]]

[[Image:RLaueBragg.png|thumb|right|250px|Reflectivities for Laue and Bragg geometries, top and bottom, respectively, as evaluated by the [[:en:Dynamical theory of diffraction|Dynamical theory of diffraction]] for the absorption-less case. The flat top of the peak in Bragg geometry is the so-called [[Darwin Plateau]]. ([http://www.kdliss.de/KDL/DissLiss/index.html Ref.])]]

====Principle of theory====

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* H. Rauch, D. Petrascheck, “Grundlagen für ein Laue-Neutroneninterferometer Teil 1: Dynamische Beugung”. , AIAU 74405b, Atominstitut der Österreichischen Universitäten, (1976)

* H. Rauch, D. Petrascheck, “Dynamical neutron diffraction and its application” in “Neutron Diffraction”, H. Dachs, Editor. (1978), Springer-Verlag: Berlin Heidelberg New York. p. 303.

* Authier, André: Dynamical theory of X-ray diffraction. IUCr monographs on crystallography, no. 11. Oxford University Press (1st edition 2001/ 2nd edition 2003). ISBN 01985289220-19-852892-2.

[[Category:Neutron related techniques]]