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The motion of chaotic oscillators cannot be uniquely parametrized by the phase in contrast to classical oscillators; however, the phase variable suffices for the determination of the location and charge of a topological defect in the spatially distributed medium
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The motion of chaotic oscillators cannot be uniquely parametrized by the phase in contrast to classical oscillators; however, the phase variable suffices for the determination of the location and charge of a topological defect in the spatially distributed medium.
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27
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85036303151
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The distortion of the local orbits by the motion of the topological defects cannot only cause the breakdown of global phase synchronization but also the breakdown of a proper phase description, i.e., no unique center of rotation exists. However, the percentage of loops in phase space, where (Formula presented) lies outside the loop is of the order of (Formula presented) for K close to (Formula presented) and, thus, extremely small. In particular, the effect on the estimate of the oscillator’s frequency is negligible
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The distortion of the local orbits by the motion of the topological defects cannot only cause the breakdown of global phase synchronization but also the breakdown of a proper phase description, i.e., no unique center of rotation exists. However, the percentage of loops in phase space, where (Formula presented) lies outside the loop is of the order of (Formula presented) for K close to (Formula presented) and, thus, extremely small. In particular, the effect on the estimate of the oscillator’s frequency is negligible.
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30
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85036261382
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These scenarios include, for example, a nonmonotonical dependence of the number of topological defects on K and fluctuations in the number of topological defects on very short time scales
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These scenarios include, for example, a nonmonotonical dependence of the number of topological defects on K and fluctuations in the number of topological defects on very short time scales.
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