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The characteristic peak frequency in Figure 3c is related to the charge transfer rate.
Expected artificial perturbations can first be seen as a peak close to the 30-Hz frequency in Figure 1.
The high sampling frequency in Figure 18 is about 20 Hz when the map size is small.
The normalized frequency in Figure 6b, c, d is presented with the resolution of f s /N, where f s is the sampling frequency.
For a driving at this best frequency, in Figure 9b we show the dependence of the sensitivity on the stimulus amplitude F0.
The pressure fluctuations on half blade passage frequency in Figure 9 show that the amplitude of the pressure fluctuation on such frequency at l.2 Qn is two times as large as that at 1.0 Qn.
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Simple visualization such as the observed frequency in Figures 1 and 2 is always helpful to avoid specifying a highly inappropriate model.
As the dashed line is lower than the real line for all frequencies in Figure 4, the noise signal has been suppressed remarkably.
The CSD algorithm began converging in a similar manner, but was not able to fully achieve the relatively high 20 dB gain required at the lowest frequencies in Figure 5.
A principal component analysis based on the ADH1B haplotype frequencies in Figure 3 was used to examine the data distribution among populations (Figure 4A).
The relationship between phase and slope can explain the slope coding observed for the stimuli with lower cut-off frequencies in Figure 6B.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com