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Figure 5
Illustration of motions required for achieving arbitrary in-plane crystal orientation φ at a given incident angle θ. The objective is to align the interested in-plane vector to the projection of the incident beam. The three steps in the dashed box are compounded into one equivalent hexapod motion.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 16| Part 6| October 2009| Pages 788-795
doi:10.1107/S0909049509037911
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