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Figure 2
The linear Doppler effect contribution due to the final width δ of the synchrotron beam, and also due to the finite distance h between the axis x and the axis of the synchrotron beam. In both cases the tangential velocity of the resonant absorber has a finite projection onto the axis of the synchrotron beam.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 25| Part 6| November 2018| Pages 1703-1710
https://doi.org/10.1107/S1600577518011815
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