Difference between revisions of "Dynamical diffraction"
From Online Dictionary of Crystallography
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== Definition == | == Definition == | ||
| − | When a crystal is perfect or nearly perfect, the usual geometrical, or [[kinematical theory]] of diffraction is an insufficient approximation and the [[dynamical theory]] of diffraction must be used to describe the diffracted | + | When a crystal is perfect or nearly perfect, the usual geometrical, or [[kinematical theory]] of diffraction is an insufficient approximation and the [[dynamical theory]] of diffraction must be used to describe the diffracted intensities. |
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== See also == | == See also == | ||
| − | Section 5.1 of ''International Tables | + | *Section 5.1 of ''International Tables for Crystallography, Volume B'' for X-rays |
| − | + | *Section 5.2 of ''International Tables for Crystallography, Volume B'' for electrons | |
| − | Section 5.2 of ''International Tables | + | *Section 5.3 of ''International Tables for Crystallography, Volume B'' for neutrons |
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| − | Section 5.3 of ''International Tables | ||
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[[Category:X-rays]] | [[Category:X-rays]] | ||
Latest revision as of 13:34, 13 May 2017
Definition
When a crystal is perfect or nearly perfect, the usual geometrical, or kinematical theory of diffraction is an insufficient approximation and the dynamical theory of diffraction must be used to describe the diffracted intensities.
See also
- Section 5.1 of International Tables for Crystallography, Volume B for X-rays
- Section 5.2 of International Tables for Crystallography, Volume B for electrons
- Section 5.3 of International Tables for Crystallography, Volume B for neutrons