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Figure 1
(a, b) k-Weighted EXAFS χ(k) function and its corresponding Fourier transform (FT) for the uranium L3-edge for the UO2(NO3)2(H2O)2 experimental data after subtracting the double-electron excitation are shown at the top of each panel (black trace). Beneath the experimental data are the contributions from each individual path of the standard model of ICSD-23825. (c) Magnitude and imaginary components of the FT for the experimental data of the UO2(NO3)2(H2O)2 powder sample and corresponding fits.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 23| Part 3| May 2016| Pages 758-768
doi:10.1107/S1600577516001910
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