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Figure 3
(a, b) 2θ angles of the Bragg diffraction with the various crystal orientations for silicon and diamond, respectively. The horizontal dashed lines represent the boundary defined by the designed angular motion range of the detector arm. (c, d) Transmissions of the spectrometer assuming a silicon crystal of 10 µm thickness or a diamond crystal of 20 µm thickness.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 23| Part 1| January 2016| Pages 3-9
doi:10.1107/S1600577515022559
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