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Figure 2
Schematic illustration of the change of beam angular size in phase space by the slope errors of an optics from σθ2 to [(\sigma_{\theta2}^2+\alpha_{\rm{s}}^2)^{1/2}], where σθ2 is the divergence only of the rays at a given surface location of the optics, not the divergence of the whole beam.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 17| Part 5| July 2010| Pages 644-652
doi:10.1107/S0909049510024337
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