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Figure 4
(a) Cut at constant qz through the NR-(111)-signal from a NR at the edge of the array. (b) Simulated intensity distribution obtained from two-dimensional fast Fourier transform of an irregular homogeneous hexagon (black inset). (c) Amplitude and phase of the diffracting NR obtained by phase-retrieval analysis of the data shown in (a).

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 16| Part 6| September 2009| Pages 796-802
doi:10.1107/S0909049509032889
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