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Figure 1
A simplified schematic of the experimental setup with two orthogonal rotation axes. The beam incidence is perpendicular to the ψ axis and the MM-PAD, and the main beam is blocked by the beamstop. The crystal is rotated in increments of 0.1° about the ψ axis, with the data frames recorded by the MM-PAD when φ traverses 360° continuously at each value of ψ. The figure is not drawn to scale.

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 50| Part 4| August 2017| Pages 985-993
https://doi.org/10.1107/S1600576717006537
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