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Figure 11
(Left panel) Resolution curves of the Si(555) strip-bent analyser with various strip widths compared with the pure bending Takagi–Taupin (TT) solution. The diameter of the analyser was set to 100 mm, the bending radius to 0.5 m and the wafer thickness to 150 µm. The Bragg angle was chosen to be 88.5° and the Johann error was neglected. (Right panel) Standard deviations/central limit theorem FWHMs of the resolution curves compared with the prediction based on the expression [\left({\sigma _{0}^{2}+\sigma^{2}} \right)^{1/2}], where σ0 is the standard deviation of the pure bending TT-solution and σ is calculated from the isotropic rectangular wafer model [equation (54[link])] with the in-plane averaged Poisson's ratio [\overline{\nu} = 0.1621].

IUCrJ
Volume 8| Part 1| January 2021| Pages 102-115
ISSN: 2052-2525