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Figure 1
Schematic of the beam monitor. A negligible part of the main X-­ray beam is scattered by a thin foil towards a linear diode array. The part of the foil visible to each individual diode element is defined by Soller slits. By changing the angle of the foil with the beam, the footprint of the X-ray can be set for optimum beam-position sensitivity.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 6| Part 6| November 1999| Pages 1071-1075
doi:10.1107/S0909049599010596
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