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Figure 1
Schematic representation of the situation in reciprocal space for asymmetric Bragg-case diffraction. After the rotation of P1P2 about the axis o parallel with a surface by an angle β, this line will intersect the sphere SpH at a point Pβ which will be the starting point of the diffracted wave vectors for general asymmetric Bragg-case diffraction. Pβ is above the plane of the drawing and its projection onto this plane coincides with P2.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 8| Part 6| October 2001| Pages 1200-1202
doi:10.1107/S0909049501014613
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