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Figure 10
The idealized detector efficiency [equation (33)[link]], taking into account the shadowing and the efficiency change due to the neutron path length within the cylindrical tube. (a) λ = 12 Å, ω = 0, (b) λ = 4.9 Å, ω = 0, (c) λ = 4.9 Å, ω = 20°, all with lateral movement of the detector xpiv = 0.5 m. The beam centre is marked with a cross. Intensities are normalized to 1.

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 50| Part 5| October 2017| Pages 1382-1394
https://doi.org/10.1107/S1600576717011463
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