2022
DOI: 10.1007/s00500-022-07608-5
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A new hyperchaotic system with Hopf bifurcation and its boundedness: infinite coexisting hidden and self-excited attractor

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Cited by 2 publications
(1 citation statement)
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“…Understanding the behavior of attractors, which characterize the long-run dynamics of these systems, is a crucial aspect of their analysis [3][4][5]. Attractors can be broadly divided into two classes: self-excited attractors, which arise from unstable fixed points [6][7][8], and hidden attractors, which arise in systems with stable fixed points [9][10][11], no equilibrium points [12], or multiple line equilibria [13]. The exploration of hidden attractors has opened up new avenues for deeper insights into and manipulation of the chaotic behavior exhibited by such systems.…”
Section: Introductionmentioning
confidence: 99%
“…Understanding the behavior of attractors, which characterize the long-run dynamics of these systems, is a crucial aspect of their analysis [3][4][5]. Attractors can be broadly divided into two classes: self-excited attractors, which arise from unstable fixed points [6][7][8], and hidden attractors, which arise in systems with stable fixed points [9][10][11], no equilibrium points [12], or multiple line equilibria [13]. The exploration of hidden attractors has opened up new avenues for deeper insights into and manipulation of the chaotic behavior exhibited by such systems.…”
Section: Introductionmentioning
confidence: 99%