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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.

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APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
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