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Figure 1
Geometry in real space of X-ray pulse diffraction in the Bragg and Laue cases. 1, incident pulse Ein(r, t); 2, transmitted pulse E0(r, t); 3, reflected pulse Eh(r, t) in the Bragg case; 4, reflected pulse in the Laue case; 5, crystal; θ0 and θh are the angle of incidence of the initial pulse and the angle of reflection of the diffracted pulse, respectively, relative to the axis z.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 15| Part 5| July 2008| Pages 495-505
doi:10.1107/S0909049508019602
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