Premium
High‐energy X‐ray diffuse scattering
Author(s) -
Ramsteiner I. B.,
Schöps A.,
Reichert H.,
Dosch H.,
Honkimäki V.,
Zhong Z.,
Hastings J. B.
Publication year - 2009
Publication title -
journal of applied crystallography
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.429
H-Index - 162
ISSN - 1600-5767
DOI - 10.1107/s0021889809011492
Subject(s) - scattering , reciprocal lattice , physics , bragg's law , diffraction , extinction (optical mineralogy) , optics , synchrotron radiation , synchrotron , biological small angle scattering , photon , wide angle x ray scattering , absorption (acoustics) , bragg peak , atomic physics , neutron scattering , small angle neutron scattering , beam (structure)
Diffuse X‐ray scattering has been an important tool for understanding the atomic structure of binary systems for more than 50 years. The majority of studies have used laboratory‐based sources providing 8 keV photons or synchrotron radiation with similar energies. Diffuse scattering is weak, with the scattering volume determined by the X‐ray absorption length. In the case of 8 keV photons, this is not significantly different from the typical extinction length for Bragg scattering. If, however, one goes to energies of the order of 100 keV the scattering volume for the diffuse scattering increases up to three orders of magnitude while the extinction length increases by only one order of magnitude. This leads to a gain of two orders of magnitude in the relative intensity of the diffuse scattering compared with the Bragg peaks. This gain, combined with the possibility of recording the intensity from an entire plane in reciprocal space using a two‐dimensional X‐ray detector, permits time‐resolved diffuse scattering studies in many systems. On the other hand, diffraction features that are usually neglected, such as multiple scattering, come into play. Four types of multiple scattering phenomena are discussed, and the manner in which they appear in high‐energy diffraction experiments is considered.