4.7 Article

Bursting oscillations with multiple modes in a vector field with triple Hopf bifurcation at origin

Journal

JOURNAL OF SOUND AND VIBRATION
Volume 545, Issue -, Pages -

Publisher

ACADEMIC PRESS LTD- ELSEVIER SCIENCE LTD
DOI: 10.1016/j.jsv.2022.117422

Keywords

Triple Hopf bifurcation; Coupling of two scales; Generalized autonomous fast subsystem; Bursting oscillation; Transformed phase portrait; Bifurcation mechanism

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This study investigates bursting oscillations in a vector field with triple Hopf bifurcation, and observes the evolution of stable limit cycles and the synchronization behavior of state variables by introducing slow-varying external excitation. An interesting finding is the quasi-periodic behavior in the three-mode bursting oscillations.
The mechanism of bursting oscillations in high dimensional systems with the coupling of two scales is an open problem in nonlinear dynamics, since there may coexist stable attractors in the fast subsystem with different bifurcations. Here we consider the bursting oscillations in the normal form up to the third order of a vector field with triple Hopf bifurcation at origin. When slow-varying external excitation is introduced, with the increase of the exciting amplitude, Hopf bifurcations in the three sub-planes occur in turn, which leads to three stable limit cycles. The dynamics may evolve from a 2-D torus bursting oscillations with two-mode and three-mode, respectively, the mechanism of which can be presented by overlapping the transformed phase portrait and the equilibrium states as well as the bifurcations of the fast subsystem. Synchronization and non-synchronization between the state variables in different sub-planes can be observed, which is explained by the bifurcations. An interesting phenomenon is found that the three-mode bursting oscillations still behave in quasi-periodic type instead of high dimensional torus. The projections of the trajectory in the sub-planes alternate between quiescence and repetitive spiking state with the oscillating frequency approximated at the frequency of the corresponding limit cycle.

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