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Figure 3
Comparison of existing Bragg magnifiers in terms of their resolution limit Δxres calculated according to the equation (3) . Each of these magnifiers works at different optimal energy Eopt (see Table 1 ). (a) Si (111) (Kobayashi et al., 2001 ); (b) our Ge (220) magnifier; (c) Si (220) (Stampanoni et al., 2006 ); (d) Si (224); (e) Si (004), α = 33.17° (Schäfer & Köhler, 2003 ; Modregger et al., 2006 ). |


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