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Weighted spectra of the fitting components (see text) are plotted as plain lines below each fitted spectrum.
Uncertainty is determined through subtracting between the original data and the fitted spectrum.
The reconstructed or fitted spectrum is displayed in the right panel of Fig. 10.
Figure 11 Nyquist plots of actual data and fitted spectrum of PPy nanotube electrodes obtained after etching ZnO core.
Figure 10 Nyquist plots of actual data and fitted spectrum of ZnO nanorod core-PPy sheath electrode.
These parameters are used to produce the fitted spectrum in Fig. 2. The mean velocity U agrees with that obtained from the ion measurements (cf. time series plot in Fig. 1), 〈u〉 = 443.0km/s, but the random sweeping velocity V is markedly large and cannot be explained simply by the root-mean-square of the ion velocity fluctuation (at about 7 km/s).
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We can now plot these fitted spectra, and look at the δχ residuals of the fit.
The optical spectra (R and T) of all single films were in a good agreement with the fitted spectra by dielectric function models.
The fitted spectra cover a range from [Formula presented] 50 TeV up to several thousand TeV.
Symbols represent experimental data and lines represent fitted spectra using equivalent circuit.
Solid and red dotted lines in A represent raw and fitted spectra, respectively.
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