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Figure 10
(a)–(d) Numerical simulations performed for the 15 different edges listed in Table 1[link]. By tuning α = α1,2 = −α3,4 of the HRM the linear dispersion rate of the source can be tuned. The dashed horizontal lines present the targeted Gsrc values.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 33| Part 1| January 2026| Pages 218-226
https://doi.org/10.1107/S1600577525010318
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