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Figure 6
(a) The calculated flux transmission through the DCD as a function of energy at φ = 0. For silicon the transmission is only 5–10% whereas this can be significantly improved by replacing the DCD crystals. (b) Maximum flux before the DCD, at a ring current of 300 mA. Collimation and windows etc. can reduce this by up to half, which, for example, gives a flux at the sample position of ∼2 × 1012 photons s−1 (0.1% bandwidth)−1 (at 12.5 keV and φ = 0).

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 19| Part 3| March 2012| Pages 408-416
doi:10.1107/S0909049512009272
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