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Figure 1
(a) Schematic of a conventional energy-dispersive RIXS setup with a diced spherical analyzer A, a strip detector D, and sample S in a Rowland circle geometry (dashed). Extrinsic elastic scattering from point S′ ≠ S arrives at the detector at F′ ≠ F and is therefore counted at a different energy. (b) Schematic of a conventional RIXS setup with a bent spherical analyzer A. Scattered X-rays from S and S′ will be focused on different single points at F and F′ and therefore do not interfere with each other.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 27| Part 4| July 2020| Pages 963-969
https://doi.org/10.1107/S1600577520005792
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