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Figure 1
Scattering geometries of a GIXD and a LEED experiment with k0 and k as the wavevector of the primary and scattered radiation, respectively. In GIXD the complete scattering vector q is obtained experimentally, which can be split into an in-plane part qxy and an out-of-plane part qz. In LEED only qxy can be determined. The investigated reciprocal lattices are plotted in red: discrete reciprocal-lattice points in the case of GIXD and Bragg rods in the case of LEED.

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ISSN: 2053-2733
Volume 78| Part 3| May 2022| Pages 272-282
https://doi.org/10.1107/S2053273322002170
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