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Figure 6
Geometrical optics simulations of DFXM images for the same phantom as used in Fig. 4 but now as a function of varying the scattering angle 2θ from the strong beam condition (Δ2θ = 0) to the weak beam condition ([\Delta 2\theta] = 600 µrad). The position of the core of the central dislocation is indicated with a red dot.

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 57| Part 2| April 2024| Pages 358-368
https://doi.org/10.1107/S1600576724001183
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