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Figure 1
(a) The nominal longitudinal mirror profile [z_{{{\rm n}}}(x)] focuses exactly the incident beam to a focal point. (b) A deliberate deformation [z_{\rm{e}}(x)] is superposed to [z_{{{\rm n}}}(x)] in order to change the intensity distribution on the focal plane. The longitudinal profile is now [z_{{{\rm m}}}] = [z_{{{\rm n}}}] + [z_{\rm{e}}].

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 25| Part 1| January 2018| Pages 123-130
https://doi.org/10.1107/S1600577517014035
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