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Figure 5
The calculated distributions of intensity arriving at the sample in the scattering plane; curve a with the mirror, and with the sample 20 mm from the monochromator crystal, and curve b without a mirror but with an 80 µm slit and with the sample 20 mm from the monochromator crystal. The noisiness in the simulation comes from the digital nature of the calculation.

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 46| Part 6| December 2013| Pages 1626-1639
https://doi.org/10.1107/S0021889813027313
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