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Figure 2
A comparison of the predictions of (a) equation (1)[link], the NTXRD result for n = 1, and (b) equation (21)[link], our result for a cubic shaped crystallite with faces aligned to the cube axes, for radiation incident at an angle [\Omega = f \times \theta_{\rm B}] for a variety of f values. Both distributions exhibit specular reflections. Whilst the NTXRD result predicts a further peak at exactly [2 \theta_{\rm B}], we find this second peak to vary in angle as described in the text.

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