2019
DOI: 10.1063/1.5079886
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Can hyperchaotic maps with high complexity produce multistability?

Abstract: In this paper, we investigate the dynamical behavior in an M-dimensional nonlinear hyperchaotic model (M-NHM), where the occurrence of multistability can be observed. Four types of coexisting attractors including single limit cycle, cluster of limit cycles, single hyperchaotic attractor, and cluster of hyperchaotic attractors can be found, which are unusual behaviors in discrete chaotic systems. Furthermore, the coexistence of asymmetric and symmetric properties can be distinguished for a given set of paramete… Show more

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Cited by 59 publications
(37 citation statements)
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“…Importantly, when the number of coexisting multiple attractors goes to infinity, such a coexistence phenomenon is defined as extreme multistability, which is closely relied on the initial conditions and has been reported in many continuous-time dynamical systems [14], [15]. Similarly, the phenomenon of multistability can be also observed in numerous discrete iterative maps of difference equations, including the kicked rotor map [2], bistable Hénon map [16], nonlinear hyperchaotic map [17], three-degree-of-freedom vibroimpact system [18], two-dimensional sine map with initialsboosted coexisting chaos [19], and two-dimensional memristive hyperchaotic maps [20]. However, such an initial condition-relied extreme multistability has not yet been found in a discrete iterative map.…”
Section: Introductionmentioning
confidence: 92%
“…Importantly, when the number of coexisting multiple attractors goes to infinity, such a coexistence phenomenon is defined as extreme multistability, which is closely relied on the initial conditions and has been reported in many continuous-time dynamical systems [14], [15]. Similarly, the phenomenon of multistability can be also observed in numerous discrete iterative maps of difference equations, including the kicked rotor map [2], bistable Hénon map [16], nonlinear hyperchaotic map [17], three-degree-of-freedom vibroimpact system [18], two-dimensional sine map with initialsboosted coexisting chaos [19], and two-dimensional memristive hyperchaotic maps [20]. However, such an initial condition-relied extreme multistability has not yet been found in a discrete iterative map.…”
Section: Introductionmentioning
confidence: 92%
“…(1) e period of LMFSR has no relation with an initial value (2) e different outputs of LMFSR are uncorrelated e maximum period of all these experiments is 65500 when code C � 0203. e whole length of feedback shift register is 16 bits, so the maximum length of the sequence should be 2 16 � 65536.…”
Section: Analysis Of the Experimentmentioning
confidence: 99%
“…However, the performance of the discrete chaotic system degrades because of the finite precision effect. Some research studies do lots of investigation to improve the performance in low-dimensional systems [11][12][13][14] and high-dimension systems [15,16]. Hua et al [13,14] proposed a novel and efficient low-dimensional chaotic system with high complexity.…”
Section: Introductionmentioning
confidence: 99%
“…Similar to the continuous chaotic systems, the discrete chaotic maps are taken as a class of important dynamical systems, which can also give rise to the phenomenon of multistability. In the past decade, the coexistence of double or multiple attractors has been found in the Hénon maps [ 17 , 18 ], the M-dimensional nonlinear hyperchaotic model [ 19 ] and the multistage DC/DC switching converter [ 20 ]. Recently, two types of simple 2D hyperchaotic maps with sine trigonometric nonlinearity and constant controllers were shown to generate initial-boosted infinite attractors along a phase line [ 21 , 22 ].…”
Section: Introductionmentioning
confidence: 99%