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Figure 5
(a) XRS spectra after subtraction of the pre-edge curve, (b) χ(k) weighted by k2 and (c) χ(r) along with fitted curves. The solid curves in (b) are k2χ(k) by backward Fourier transformation of χ(r) in the 0.8–2.5 Å r-range. The thin curve in (c) is χ(r) by theory with an adjustment of peak height while dotted curves are by four-parameter fitting. Broken curves in (b) and (c) are window functions in forward and backward Fourier transformations.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 20| Part 2| January 2013| Pages 266-271
doi:10.1107/S0909049512048789
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