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Figure 1
Validation of our method using numerical simulations. (a) g(r) is the theoretical curve built using three Gaussian peaks with n1 = n2 = n3 = 2, r1 = 1.923, r2 = 2.012, r3 = 2.086, [\sigma^2] = 0.005. [\Delta r_1] is the bond length difference between r1 and r2. [\Delta r_2] is the bond length difference between r2 and r3. To resolve these three peaks, a spatial resolution better than the smallest one, [\Delta r_2], is needed. These three peaks merged into a single peak which is indistinguishable using existing EXAFS data analysis methods. (b) Simulated data are the EXAFS data [\chi(k)] calculated using equation (1)[link] with added noise. Data are k3-weighted. The fitting curve is the curve fitted by our algorithm. A Hanning window for the FT is shown as a dashed line and the window parameter is 20. (c) The dashed line shows the phase- and amplitude-corrected FT spectrum (van Zon et al., 1984BB33) of the simulated data. The three peaks are indistinguishable using this method. The solid line shows the atom distribution function (ADF) calculated from our method. The peaks are clearly resolved. The peak position and the area are the bond length and coordination number, respectively. Calculated parameters are n1 = 2.0, n2 = 2.1, n3 = 2.0, r1 = 1.915 Å, r2 = 2.007 Å, r3 = 2.082 Å, [\sigma^2] = 0.0049 Å2, which are very close to the true values.

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
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