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Figure 8
Spatial distribution of the incident count rate for the fundamental energy [(a) and (c)] and the first harmonic [(b) and (d)] using the detuned second crystal of the MLM-Ru [ES2, (a) and (b)] and MLM-V [ES4; (c) and (d)]. These count rates are corrected for the attenuation of the beam by the filters and the detection efficiency of the 450 µm-thick sensor of the SLcam. The high-intensity regions at the top of the image are due to incomplete filtering of the field-of-view.

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