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![[Figure 2]](https://journals.iucr.org/tv5013fig2mag.jpg)
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| Figure 2 Averaged Bragg-plane slope errors ![[\langle \sigma _{\theta}\rangle]](https://journals.iucr.org/10.1107/S1600577520012746/teximages/tv5013fi3.gif) (a) and normalized dispersions ![[\langle \Sigma _{\Delta\theta}\rangle]](https://journals.iucr.org/10.1107/S1600577520012746/teximages/tv5013fi8.gif) of the Bragg reflection widths (b) for the reference Si crystal in the 531 Bragg reflection measured and calculated
as a function of the area-detector binning number N. The averaging is performed in one of three ways over 16 equal-sized 1 mm × 1 mm
crystal's ROIs, over four 2 mm × 2 mm ROIs, or just calculated in one 4 mm × 4 mm
ROI, as indicated by red, black and blue lines, respectively, in (a) and (b) and on the X-ray Bragg diffraction image in (c). |
![[Figure 2]](https://journals.iucr.org/10.1107/S1600577520012746/tv5013fig2.jpg)
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JOURNAL OF SYNCHROTRON RADIATION |
ISSN: 1600-5775
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