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Figure 2
Left: intensity as a function of phase-plate Bragg angle (θpp) for a 400 µm-thick diamond phase plate at 6.971 keV, measured at the (−1, 1, −1) reflection. The polarization of the transmitted intensity was analysed using a Cu (2, 2, 0) polarization analyser at analyser angles of 0° (blue) and 90° (red). Left inset: monochromatic topographical image of the 1000 µm-thick diamond phase plate highlighting the excellent quality of the monosectorial plate. Right: continuous rotation of linearly polarized light with a 1000 µm-thick diamond phase plate at 7 keV as a function of the rotation angle of the phase retarder crystal, χpp. |

journal menu![[Figure 2]](mad5008fig2.jpg)
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