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Figure 6
(a) Diffraction curve simulated for a pair of SFs, using the effective coherence width of Lcoh = 2 µm, and the SF positions z1 and z1 + 200dWZ = z1 + 65.6 nm; the rectangles represent the Qz-windows used for the simulation of the Patterson functions in panels (b) and (c). (b) The Patterson functions calculated for various distances z2-z1 = [(200+\Delta n)d_{{\rm WZ}}] of the I1–I1 SF pair. The parameters of the curves correspond to the numbers of the Qz-windows in panel (a); the colours of the curves denote the values of [\Delta n]. (c) The Patterson functions calculated for the same SF positions but different SF types; the types of the SFs correspond to different colours of the curves. The curves corresponding to different Qz-windows are shifted vertically.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 24| Part 5| September 2017| Pages 981-990
https://doi.org/10.1107/S1600577517009584
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