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Figure 11
(a) The calculated dispersion of the scattering power in Ω and X as a function of 2θ (effectively the integral of Fig. 7[link] without oversampling from axial divergence). (b) The calculated integrated intensity in Ω and X as a function of 2θ with the variable axial divergence limited by Soller slits as in an experiment (equivalent to the integral of Fig. 7[link] with oversampling).

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