Computer simulations of X‐ray spherical wave dynamical diffraction in one and two crystals in the Laue case. Issue 6 (12th October 2018)

• Record Type: Journal Article
• Authors: Kohn, V. G.; Smirnova, I. A.
• Is Part Of: Acta crystallographica. Volume 74:Issue 6(2018:Nov.)
• Page Start: 699
• Page End: 704
• Publication Date: 2018-10-12
• Subjects: X‐ray diffraction -- diffraction focusing -- compound refractive lens -- synchrotron radiation -- XFEL energy spectrometer; Crystallography -- Periodicals; Condensed matter -- Periodicals; 548
• DOI: 10.1107/S2053273318012627
• Languages: English
• ISSNs: 2053-2733

Abstract

Abstract : Computer simulations of X‐ray spherical wave dynamical diffraction in one and two crystals in the Laue case are reported. A spherical wave is created by an X‐ray compound refractive lens. Diffraction focusing phenomena in one crystal and for the reflected beam, as well as in two crystals and for the twice‐reflected beam, are simulated and discussed. How these phenomena may be used in an energy spectrometer is investigated. Abstract : This article reports computer simulations of X‐ray spherical wave dynamical diffraction in one and two single crystals in the Laue case. An X‐ray compound refractive lens (CRL) as a secondary radiation source of spherical waves was considered for the first time and in contrast to previous simulations with the assumption of the use of a slit. The main properties of the CRL as a secondary source are discussed and two focusing phenomena are analysed. The first one is the diffraction focusing effect for one single crystal in the reflected beam and in the case of a large source‐to‐detector distance. The second one is the same but for two single crystals and for the twice‐reflected beam in the case of a short distance between the source and detector. The first effect is well pronounced in the case of strong absorption. However, it may also be used as an element of an energy spectrometer in the medium and even weak absorption case. The second effect will appear in the case of weak absorption. It is shown that it is not effective to use it in an energy spectrometer. In the case of weak absorption the transverse size of the diffraction focused beam will oscillate together with the reflected beam integral intensity. The oscillation period is close to the extinction length.