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The other is the problem of spectra components interference between the two components in adjacent frequency bins [19, 20]. Figure 1 presents an example that demonstrates the drawbacks of the DFT.
Second, there exists the problem of spectra components interference at a, b, c, and d frequency bins, because the corresponding accurate frequencies at A, B, C in Figure 1b are too adjacent to each other.
The elemental concentrations based on the relative area of XPS spectra components for Co 2p, Mo 3d, Si 2p and O 1s were obtained for the surface of CoHPM/silica.
The matrix was then deconvoluted using the CCA module as previously described [42], [71], yielding a predefined number, P, of base spectra components.
On the other hand, the MP coefficients well represent the frequency components without the problem of the spectra components interference, such as these components at A, B, and C shown in Figure 2d, but the DFT coefficients fail to do this even in the noise-free case.
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However, NHA does not reveal the spectrum components of a sound in the side lobes.
2I + 1 is the number of spectrum components within one range-Doppler bin.
The other part related to along-track position errors changes with spectrum components.
In particular, this scheme converges uniformly for both continuous and discrete spectrum components.
In addition to molecular structure graphics, spectrum components can display NMR, IR, UV/Vis and mass spectrometry spectra.
Then, phase errors are estimated by using the spectrum components within the zero Doppler bin as calibration sources.
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