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Figure 4
While there might be practical limitations to the number of zone plates nzp that can be stacked together, one can obtain gains in first-order diffraction efficiency [\varepsilon_{1}] that go well beyond the simple thin zone plate expression of equation (1)[link]. In (a) we show the efficiency as a function of individual zone plate thickness ti and cumulative thickness t, where nzp = t/ti zone plates are used with with a separation of [\Delta z] = 10 µm (for d = 45 µm, and drN = 25 nm for the first zone plate at 10 keV). A single gold zone plate with the optimum thickness topt = 2.0 µm would give [\varepsilon_{1}] = 32.7%, whereas much higher efficiencies can be obtained by using many more zone plates with slightly higher cumulative thickness. In (b) we show how the stacking of nzp = 8 zone plates, each with a thickness ti = 0.5 µm, leads to differences in diffraction efficiency as one changes the separation distance [\Delta z] between zone plates. Smaller separation distances [\Delta z] are preferable but might be impractical, but even with larger separation distances like [\Delta z] = 1000 µm one can still obtain an efficiency of [\varepsilon_{1}] = 36% if nzp = 5 zone plates are used. All calculations were for gold zone plates at 10 keV.

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SYNCHROTRON
RADIATION
ISSN: 1600-5775
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