As shown in the Bode phase plots, the modification of the silicon surface allows the increase of the phase angle at high frequencies for both deposition techniques, being higher for the sample grafted with five CV cycles.
However, despite this imposed kinematic relationship, the phase plot between the cumulative spike count of the SC cell and the actual eye displacement was not invariant to the temporal changes in the SC burst.
The two-parameter phase plot shows the projection of the burst trajectory onto the slow variable n o plane.
To obtain a clearer picture of the behaviour of the module, we created a phase plot of the concentration of the response at adjacent spatial locations.
The Bode phase plot of the samples were also conducted to further demonstrates the lower recombination of the photogenerated carriers.
Figure 3 shows the simulation results of the amplitude and phase plot for the composite electromagnetic wave.
A phase plot of the concentration of the response at two adjacent spatial points no longer shows a filled region but a closed curve indicating that the oscillations at different points in space are now synchronized with one another.
These data were interpreted as evidence for entrainment, yet both the slope in the peak phase plots and the differences in the timing of the conidiation peaks are consistent with the depicted hourglass mechanism.
Figure 2 Phase plot for the VOFVDPM with different linear variable-order functions, (pmb{a=0}), (pmb{mu=2.5}), and (pmb{(x 0),y(0))=(1.3,1.2)}).
The phase plots show the behavior of the dynamical system in modes 1 and 3.
