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 that go well beyond the simple thin zone plate expression of equation (1). 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 = 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 = 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 between zone plates. Smaller separation distances are preferable but might be impractical, but even with larger separation distances like = 1000 µm one can still obtain an efficiency of = 36% if nzp = 5 zone plates are used. All calculations were for gold zone plates at 10 keV. |