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Dynamics of Lu et al.’s fractional-order system with the order α=0.95, in context of x, y, and z directions.

Dynamics of Lu et al.’s fractional-order system with the order α=0.95, in context of x, y, and z directions.

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In this paper, we consider a class of fractional-order systems described by the Caputo derivative. The behaviors of the dynamics of this particular class of fractional-order systems will be proposed and experienced by a numerical scheme to obtain the phase portraits. Before that, we will provide the conditions under which the considered fractional-...

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The dynamics of the Caputo-fractional variable-order difference form of the Tinkerbell map are studied. The phase portraits, bifurcation, and largest Lyapunov exponent (LLE) were employed to demonstrate the presence of chaos over a different fractional variable-order and establish the nature of the dynamics. In addition, the 0–1 test tool was used...

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... It is essential to emphasize that fractional-order differentiators have two primary operators, the Riemann-Liouville derivative operator and the Caputo derivative operator, which are both methods that relate to the local derivative of a function [11]. The Caputo differentiator has been shown to be superior to the Riemann-Liouville differentiator for a number of real-world applications [12,13], despite the divergent views of many mathematicians [14,15]. This is because it can be used with certain supposed initial conditions once taking the derivatives of fractional-order [16,17]. ...
... In this regard, we assume that we want to find an approximate value for J α a f (x) when α = 0.85 and α = 1 over the interval [0, 1] by choosing subintervals' number as n = 8. Observe that the values of J α a f (x) when α = 0.85 and α = 1 that could be obtained using Ortigueira et al. [23] or formula (13) can be viewed in Table 2. It should be noticed here that the last two approximated values generated in Tables 3 and 4 using the proposed composite fractional Trapezoidal rule with Romberg integration are very close to the values of J α a f (x) obtained using formula (13) reported in Table 2. ...
... Observe that the values of J α a f (x) when α = 0.85 and α = 1 that could be obtained using Ortigueira et al. [23] or formula (13) can be viewed in Table 2. It should be noticed here that the last two approximated values generated in Tables 3 and 4 using the proposed composite fractional Trapezoidal rule with Romberg integration are very close to the values of J α a f (x) obtained using formula (13) reported in Table 2. In particular, one can find the absolute values of the errors gained from the two approaches to be as 0.011257 and 0.002916 for α = 0.85 and α = 1, respectively. ...
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... Eventually, the validity of the theoretical results was verified by three numerical simulations. In addition, some of the issues discussed in [36][37][38] (fractional-order chaotic or hyperchaotic systems, synchronous ...
... Eventually, the validity of the theoretical results was verified by three numerical simulations. In addition, some of the issues discussed in [36][37][38] (fractional-order chaotic or hyperchaotic systems, synchronous communication of fractional-order chaotic systems, and event-triggered impulsive chaotic synchronization of fractional-order systems) are also interesting and will be further considered in future work. ...
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... Before the motivations and the works described in this paper, we give a brief literature review concerning modeling chaotic systems with and without fractional-order derivative. Recently, Sene et al. introduce several fractional chaotic systems via Caputo derivative and study their phase *Corresponding Author portraits, bifurcations diagrams, Lyapunov exponents, sensitivity to the initial conditions, and influence of the fractional orders in obtaining new types of attractors, see in the following investigations [11,14,[16][17][18]. In [13], In the fractional context, Pacheco et al. introduce and investigate fractional chaotic systems with hidden and selfexcited attractors. ...
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... e theory of differential equations of arbitrary order has been recently proved to be an important tool for modeling many physical phenomena. For more details, refer to [4][5][6][7][8][9]. e fractional integro-differential equations have been recently used as effective tools in the modeling of many phenomena in various fields of applied sciences and engineering such as acoustic control, signal processing, electrochemistry, viscoelasticity, polymer physics, electromagnetics, optics, medicine, economics, chemical engineering, chaotic dynamics, and statistical physics (see [10][11][12][13][14][15][16]). ...
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