2015
DOI: 10.1007/s11071-015-2520-4
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Bifurcations at infinity, invariant algebraic surfaces, homoclinic and heteroclinic orbits and centers of a new Lorenz-like chaotic system

Abstract: We present a global dynamical analysis of the following quadratic differential systeṁ x=a(y−x),ẏ = dy − xz,ż =−bz + f x 2 + gx y, where (x, y, z) ∈ R 3 are the state variables and a, b, d, f, g are real parameters. This system has been proposed as a new type of chaotic system, having additional complex dynamical properties to the well-known chaotic systems defined in R 3 , alike Lorenz, Rössler, Chen and other. By using the Poincaré compactification for a polynomial vector field in R 3 , we study the dynamics … Show more

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Cited by 6 publications
(4 citation statements)
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“…is a polynomial first integral of system (1), where f i are the homogeneous polynomials of degree i and f n ̸ = 0. Firstly, substituting (11) into (10) and identifying the homogeneous components of degree n + 1, we get…”
Section: Homothetic Transformation Between the Gd Model And Other Qua...mentioning
confidence: 99%
See 1 more Smart Citation
“…is a polynomial first integral of system (1), where f i are the homogeneous polynomials of degree i and f n ̸ = 0. Firstly, substituting (11) into (10) and identifying the homogeneous components of degree n + 1, we get…”
Section: Homothetic Transformation Between the Gd Model And Other Qua...mentioning
confidence: 99%
“…To this end, in this section we will analyze the Poincaré compactification of the GD model in the local charts U i and V i (i = 1, 2, 3). We refer to [10], [7], [11], [25] for the detailed theory of Poincaré compactification.…”
Section: Co-dimension Two Bifurcationsmentioning
confidence: 99%
“…To do this, in the next three subsections we shall analyze the Poincaré compactification of system (6) in the local charts U i and V i (i = 1, 2, 3). The detailed theory of Poincaré compactification can be found in [10], [11], [12], [13].…”
Section: Theorem 23 (Existence Of Hopf Bifurcation) Assume That (Hmentioning
confidence: 99%
“…In Section 4, we contribute to investigating the global dynamics of the QPP model by studying its behavior at infinity. Since the QPP model is a polynomial vector field in R 3 , by the Poincaré compactification one can extend the QPP model into an analytic system defined on a closed ball of radius one, called the Poincaré ball, whose interior is diffeomorphic to R 3 and its invariant boundary, the twodimensional spherical shell S 2 = {(x, y, z)|x 2 + y 2 + z 2 = 1} plays the role of the infinity, called the Poincaré sphere [10], [11], [12], [13]. Using this compactification technique, we give a complete description of the dynamical behavior of the QPP model on the sphere at infinity (Theorem 4.1).…”
mentioning
confidence: 99%