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Ming-Chi Lu, Hsing-Chung Ho, Chen-An Chan, Chia-Ju Liu, Jiann-Shing Lih, Ming-Chung Ho, "Phase Synchronization Is the Amplified Result by the Hilbert Transform", Mathematical Problems in Engineering, vol. 2015, Article ID 640107, 3 pages, 2015. https://doi.org/10.1155/2015/640107
Phase Synchronization Is the Amplified Result by the Hilbert Transform
We investigate the interplay between phase synchronization and amplitude synchronization in nonlinear dynamical systems. It is numerically found that phase synchronization intends to be established earlier than amplitude synchronization. Nevertheless, amplitude synchronization (or the state with large correlation between the amplitudes) is crucial for the maintenance of a high correlation between two time series. A breakdown of high correlation in amplitudes will lead to a desynchronization of two time series. It is shown that these unique features are caused essentially by the Hilbert transform. This leads to a deep concern and criticism on the current usage of phase synchronization.
Synchronization of chaotic systems has been an important area in nonlinear dynamics . “Synchronization” is defined as a complete coincidence of two variables (or time series) that are belonging to different systems  while the appearance of some functional relations between two variables is termed as “generalized synchronization” [3, 4]. Instead of focusing on the synchronization of time series, Rosenblum et al. introduced the concept of phase synchronization to describe how the coupled chaotic oscillators could present a nearly perfect locking of phase, whereas the amplitude remained chaotic . In , the phase of a time series was defined based on the Hilbert transform . This definition is also very attractive in characterization of chaos . In a more explicit form, the Hilbert transform of a time series follows:where P.V. means the Cauchy principal value for the integral. Thus, a new complex quantity can be introduced; that is,where is the phase and is the amplitude [5, 7] and they form a conjugate pair. One can also define the phase angle to be the projection of phase point on the x-y plane with the phase angle and the amplitude . Alternatively by using the Poincare section, one can also choose a phase:where and denotes the th crossing, but there is no conjugate amplitude for . In this comment, we reexamine the virtue of using the phase variable as the indicator of synchronization of the time series. We believe that phase synchronization may not be a good tracer to the actual synchronization of the time series. Then our work will explain the onset mechanism of phase synchronization and it leads to a deep concern on the current usage of phase synchronization.
2. Give an Example of Coupled Rossler Model
Let us recalculate the same coupled Rossler model as in  to explore the synchronization. The model follows:where is the strength of coupling, , and which indicates that there is a frequency mismatch between two oscillators. Because of finite frequency mismatch, there is no exact synchronization in time series. Synchronization can be found for not only in the range , as reported in , region I, but also in , region II. Thus, in such a case, “synchronization” only implies a high correlation between two variables, such as time series. By using the Hilbert transform, the variables have the phase and the amplitude . It has been reported that and move together and get nearly synchronized, while and remain irregular and unrelated in a range of small C . Since then, cited and extended works have been expanded dramatically [8–19]. However, it should be emphasized that as phase is introduced, the influence of its counterpart, that is, amplitude, and their interplay should not be ignored. Unfortunately, although the concept of phase synchronization has been extensively addressed, the correlation between phase synchronization and amplitude synchronization remains to be clarified.
3. Results and Discussion
Let us use a common measure, the mean square error, to quantify the degree of synchronization. For two time series, and , the mean square error is defined aswhere the integration time should be sufficiently long. For the phase and the amplitude deduced by the Hilbert transform, we denote their mean square errors to be and . For phase angle defined by projection (here and of the Rossler model), the corresponding mean square errors are and , while in the case of the Poincare section (here a typical section in the plane) we use to denote it. Obviously, to be good indicators of the synchronization, variations of these quantities should faithfully reflect the true status of the coupled chaotic oscillators. As shown in Figure 1, where the values of the mean square errors in region I are plotted, the mean square errors of the phase variables are insensitive to the true state of synchronization in time series. In contrast, the mean square errors of the conjugate amplitudes reflect more faithfully to the status of oscillators in this case. Similar feature can also be found in region II as well as for different coupled oscillators.
The result shows that phase synchronization will intend to be established earlier than amplitude synchronization under the Hilbert transform. This unique feature is novel, but it is caused by the Hilbert transform. The transformation on the phase part is nonlinear. This nonlinear transform is the generic mechanism for the novel features that have been reported on the phase synchronization [5, 6, 8–19]. Therefore, we believe the role of “phase” and phase synchronization may not be a good indicator to the true synchronization in the time series. The relevance of phase variables to the synchronization of the original variables in nonlinear dynamical systems seems to be a mathematical consequence of the transform one used. Thus, the works on phase synchronization [6, 13–19] may be worthwhile to be reconsidered.
Conflict of Interests
There is no conflict of interests related to this paper.
The authors would like to thank the National Science Council, Taiwan, for financially supporting this research under contract no. NSC 102-2112-M-017-002-.
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