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Figure 3
(a) Simulation of the DCM beam after focusing (the parameters can be seen in Fig. 1[link]). No slope error was introduced to the mirrors but the image of the beam was recorded a few millimetres off the focal point to obtain a finite beam size. (b) The same configuration as in (a) after inserting the HRM into the beam. The vertical size of the beam increases from 15 µm to 80 µm and acquires an energy dispersion in the vertical direction.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 27| Part 2| March 2020| Pages 538-544
https://doi.org/10.1107/S1600577519017119
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