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. 2022 Mar 18;55(Pt 2):329–339. doi: 10.1107/S1600576722001261

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© Alberto Leonardi et al. 2022

This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.

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Reduced PDF G(r) and powder intensity profiles from hollow-shaped crystals. (a), (b) Reduced PDF and negative shape function , which is the correction term in equation (6), for powders of particles with hollow spherical (a) and hollow cubic (b) shapes. The corresponding powder intensity profiles are shown in (c) and (d). SAS particle shape contributions to the intensity profiles (red) are compared with powder intensity profiles simulated with the DSE (grey) and the WPDFM (black) method.

Inline graphic — Reduced PDF G(r) and powder intensity profiles from hollow-shaped crystals. (a), (b) Reduced PDF and negative shape function , which is the correction term in equation (6), for powders of particles with hollow spherical (a) and hollow cubic (b) shapes. The corresponding powder intensity profiles are shown in (c) and (d). SAS particle shape contributions to the intensity profiles (red) are compared with powder intensity profiles simulated with the DSE (grey) and the WPDFM (black) method.