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Figure 5
(a) The angular dependence of diffraction intensity as function of time is given for the case of a rotation over 45°. There is only a single diffraction peak that, after delay, starts to move back slowly to the original position. (b) shows an example which is representative of rotations of angles between 45 and 90°. It is clear that the behaviour is much more chaotic.

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 40| Part s1| January 2007| Pages s52-s56
doi:10.1107/S0021889806054823
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