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Figure 6
(a) Information gain (KDN estimate) as a function of maximum momentum transfer Qz,max and counting time t of the measurement for the model structure shown in Fig. 2[link] and related structures in which all layer thicknesses were multiplied by 1/2 (b) and 2 (c). The counting times shown apply to Qz,max = 0.26 Å−1, but were shorter and longer for smaller and larger Qz,max, respectively, as we have chosen an optimization scheme that preserves the counting statistics for individual data points, but not the total counting time when varying Qz,max.

Journal logoJOURNAL OF
APPLIED
CRYSTALLOGRAPHY
ISSN: 1600-5767
Volume 52| Part 1| February 2019| Pages 47-59
https://doi.org/10.1107/S1600576718017016
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