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Figure 7
Reciprocal-space coverage of the ME-GID and HE-GID experiments depending on the scattering vector length d* = [2\sin(\theta/\lambda)], where θ is half of the diffraction angle and λ is the wavelength. For better comparability, the empty areas in the detector gaps of the ME-GID experiment were classified as observed and the V-shaped blind regions were kept unfilled in both cases. The influence of the blind regions on the data completeness at a given scattering vector length is evident in the ranges up to ∼0.9 Å−1 for ME-GID and ∼2.3 Å−1 for HE-GID. Note that the blind region has almost no effect on the HE-GID coverage, while it is very significant for the ME-GID case.

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 58| Part 4| August 2025| Pages 1417-1427
https://doi.org/10.1107/S1600576725005837
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