4.7 Article

Designing Hyperchaotic Systems With Any Desired Number of Positive Lyapunov Exponents via A Simple Model

Journal

Publisher

IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC
DOI: 10.1109/TCSI.2014.2304655

Keywords

Circumferential distribution of eigenvalues; closed-loop cascade-coupling; dissipative system; hyperchaotic system; Lyapunov exponent

Funding

  1. National Science and Technology Major Project of China [2014ZX10004-001-014]
  2. 973 Project [2014CB845302]
  3. National Natural Science Foundation of China [61025017, 11072254, 61172023, 61203148]
  4. Natural Science Foundation of Guangdong Province [S2011010001018]
  5. Specialized Research Foundation of Doctoral Subjects of Education Ministry [20114420110003]
  6. Hong Kong Research Grants Council under GRF Grant [CityU 1109/12]

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This paper introduces a new and unified approach for designing desirable dissipative hyperchaotic systems. Based on the anti-control principle of continuous-time systems, a nominal system of n (n >= 5) independent first-order linear differential equations are coupled through all state variables, making the controlled system be in a closed-loop cascade-coupling form, where each equation contains only two state variables therefore the system is quite simple. Based on this setting, a simple model for dissipative hyperchaotic systems is constructed, with an adjustable parameter which can ensure the dissipation of the system. In the closed-loop cascade-coupling form, it is shown that all the eigenvalues are symmetrically distributed in a circumferential manner. Consequently, a universal law is derived on the relationship of the number of positive Lyapunov exponents and the number of positive real parts of its Jacobian eigenvalues. For the above-mentioned simple model, the number of positive Lyapunov exponents for any n-dimensional dissipative hyperchaotic system is given by N = round((n-1)/2), n >= 5. Therefore, in theory, the system can generate any desired number of positive Lyapunov exponents as long as the dimension of the system is sufficiently high. Thus, the proposed method provides a new approach for purposefully constructing desirable dissipative hyperchaotic systems. Finally, two examples are given to demonstrate the feasibility of the proposed design method.

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