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Figure 15
(a) The intensity measured in the vicinity of the 220 Bragg peak from a crystallite by isolating it from a larger diffraction space map, measured by Patricia Kidd. The geometry used was the Beam-Selection-Diffractometer (Fewster, 2004BB18), with a 100 µm double pinhole, Cu Kα and 220 Ge analyser crystal. The near-perfect match of the reflection choices removes the wavelength dispersion to reveal the intrinsic width of the Bragg peak, which is 0.002°. Along Ω is blurred by diffuse scattering and the pinhole geometry. This can be compared with Fig. 7[link], although this extremely high resolution diffraction space map is truncated because of the limited acceptable axial divergence. The maximum intensity is ∼2 counts s−1. (b) is the projected sum of the central region of the map.

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