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Figure 7
Comparison of the experimental (3ν1)* and (3ν2)* rods of diffuse scattering (compare Fig. 2[link]). Splitting of the Bragg reflections at ν = −2 and [\nu=-2{{1} \over {2}}] is due to a small secondary domain, also seen in Fig. 2[link].

Journal logoSTRUCTURAL SCIENCE
CRYSTAL ENGINEERING
MATERIALS
ISSN: 2052-5206
Volume 79| Part 6| December 2023| Pages 510-518
https://doi.org/10.1107/S2052520623009162
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