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Figure 7
The calculated intensities as Ω and X are varied for a detector at 2θ = 60° (a) and 2θ = 110° (b) for 10 µm crystallites. The intensity distribution is evaluated by randomly sampling Ω and X positions, 71 262 in (a) and 82 362 in (b), and integrating over ΔΩ and ΔX associated with the instrument function. The bounds of the instrument function, based on 0.04 radian Soller slits and diffractometer radius of 320 mm, are given by the crosses in the expanded region close to the `specular condition', Ω = θ.

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ISSN: 2053-2733
Volume 70| Part 3| March 2014| Pages 257-282
doi:10.1107/S205327331400117X
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