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Figure 3
Slices of the reconstructed reciprocal space of the SnGe4N4O4 phase of Cr1_HH228. (a) Viewing direction [110] showing the [h{\bar h}0l] reflections. For 000l reflections, l = 2n is clearly visible, no other extinctions are visible. (b) Viewing direction [[1{\bar 1}0]] showing the [hh{\overline {2h}}l] reflections, l = 2n is only violated by weak reflections. The grid shown in the figures represents the corresponding projections of the reciprocal unit cell onto the image plane. As a* and b* are not parallel to this plane in the given viewing directions, the grid points representing the projection of a* or b* onto the image plane are not occupied by reflections in the zero layer of the reciprocal space, however in higher layers above and below.

Journal logoSTRUCTURAL SCIENCE
CRYSTAL ENGINEERING
MATERIALS
ISSN: 2052-5206
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