Stability and Projective Synchronization in Multiple Delay Rössler System
|
|
- Julian Lynch
- 5 years ago
- Views:
Transcription
1 ISSN (print), (online) International Journal of Nonlinear Science Vol.7(29) No.2,pp Stability and Projective Synchronization in Multiple Delay Rössler System Dibakar Ghosh Department of Mathematics,Dinabandhu Andrews College Garia, Calcutta- 7 84, India (Received 7 August 28, accepted 1 November 28) Abstract: In this paper, the issues of projective synchronization of unidirectional coupled multiple delay systems via linear observer is investigated. A detail stability analysis of multiple delay Rössler system is derived by D-subdivision method. In the previous study, whereas projective synchronization is investigated by nonlinear observer approach, here we can achieve projective synchronization via linear observer approach. The proposed technique has been applied to synchronize multi delay Rössler system by numerical simulation. Key words: multidelay Rossler system; D-subdivision method; projective synchronization ; linear observer 1 Introduction Chaos theory has been extensively studied in various research fields after Lorenz s observation of the chaotic phenomenon [1]. Over the last decade, great attention has been paid to the dynamics of delay differential equation(dde). It has been found that the time delays not only make the systems retarded, but also are often sources of complex behaviors, like, limit cycle, loss of stability, bifurcation and chaos. So there is a growing need to depend our understanding on their complexity, particularly when multiple time delays is present. The systems with single time delay have been intensively studied but investigation of DDE s with multiple time delays has been paid little attention too. Some work has been done relative to stability analysis [2], but more complex dynamics, such as limit cycle, bifurcation and chaos in DDEs with multiple time delays, are still unclear. Chaos synchronization has received increasing attention in the last years. The phenomena of synchronization in coupled systems have been extensively studied in the context of laser dynamics, electronics circuits, chemical and biological systems [3, 4]. Over the past decade, following complete synchronization(cs) [3, 5], several new types of synchronization have been found in interesting chaotic systems, such as generalized synchronization(gs) [6], phase synchronization(ps) [7], lag synchronization(ls) [8], anticipatory synchronization(as) [9], anti-phase synchronization(aps) [1] and multiplexing synchronization [11] etc. Amongst all kinds of chaos synchronization, projective synchronization, characterized by a scaling factor that two systems synchronize proportionally, is one of the most interesting problems. This type of synchronization was first reported by Mainieri and Rehacek [12] in 1999, where they declared that the two identical systems could be synchronized up to a scaling factor α. The scaling factor is a constant transformation between the synchronized variables of the master and slave systems. Projective synchronization is not in the category of GS because the slave system of projective synchronization is not asymptotically stable. CS and APS are special cases of projective synchronization where α = 1 and α = 1 respectively. The response system attractor possesses the same topological characteristic (such as Lyapunov exponents and fractal dimensions) as the slave system attractor [13]. Projective synchronization is interesting because of its proportionality between the synchronized dynamical states. In applications to secure communications, this feature can be used to M-nary digital communication for achieving fast communication. Recently, Corresponding author. address: drghosh math@yahoo.co.in Copyright c World Academic Press, World Academic Union IJNS /219
2 28 International Journal of Nonlinear Science,Vol.7(29),No.2,pp Li et al.[14] proposed generalized projective synchronization between two different chaotic systems using combination of active control and backstepping method. Very recently, Grassi and Miller [15] introduced projective synchronization of time-delay, continuous time and discrete-time system via linear observer. In Ref. [16], Grassi and Mascolo proposed nonlinear observer design to synchronize hyperchaotic systems. An observer [16] is a dynamic system designed to be driven by the output of another dynamic system (plant) and having the property that the state of the observer converges to the state of the plant. In this paper, we discuss the details stability analysis of multiple delay Rössler system. Here we consider Rössler system with two linear time delays which occur in active sensing problems where a signal is transmitted and received at a later time. Then projective synchronization of unidirectionally coupled multidelay Rössler system is investigated with the help of linear observer(not nonlinear observer approach). The general theory for any multidelay system are investigated analytically. The effectiveness of the proposed method is verified numerically, which can also be used for other time-delayed systems. This synchronization is very much applicable in cryptography for fast communication. Recently, chaotic time delay system has been suggested as a good candidates for secure communication [17, 18]. It is proved that low dimensional chaotic systems do not ensure a sufficient level of security for communications, as the associated chaotic attractors can be reconstructed with some effort and the hidden message can be retrieved by an attacker. In this regards, time-delayed system received a lot of attention. With increases time-delay, the system is more complex and number of positive Lyapunov exponents increases and the system eventually transits to hyperchaos. The rest of this paper is organized as follows. In section 2, we will discuss stability analysis of multiple delay Rössler system. In section 3, a general theory for projective synchronization is derived by linear observer approach and verify by numerically. Finally, conclusions are made in the last section. 2 Mathematical model and bifurcation analysis A double delayed Rössler system [19] is written as ẋ = y z + α 1 x(t τ 1 ) + α 2 x(t τ 2 ), ẏ = x + β 1 y, ż = β 2 + z(x γ) (2.1) where delay parameters are τ 1 and τ 2 (τ 1 τ 2 ) and the geometric factors are α 1, α 2 while β 1, β 2, γ are the usual parameters of a standard Rössler system [2]. To start with we determine the fixed points of the system, written as; E i = (x i, y i, z i ) i)e 1 = ii)e 2 = ( ) β 2 β 1 X +, X +, β 1 X + + γ ( ) β 2 β 1 X, X, β 1 X + γ where X ± = γa± γ 2 A 2 4Aβ 1 β 2 2Aβ 1 and provided γ 2 A 2 4Aβ 1 β 2 along with A = 1 + (α 1 + α 2 )β 1. The characteristic equation of the linearized equation [19] is given by (α 1 e λτ 1 + α 2 e λτ 2 λ){λ 2 + λ(γ x β 1 ) β 1 (γ x )} = λ(1 + z ) + (γ x β 1 z ) (2.2) In[19] we have studied the special case either α = or α 2 =. To find the explicit expressions of the critical boundaries, let λ = a + ib be the root of the characteristic equation (2.2) where a and b are real. Without any loss of generality, one can assume that b >, since the roots of equation (2.2) always appear in complex conjugate pairs. If τ 1 = τ 2 = τ, then the equation (2.2) becomes {(α 1 + α 2 )e λτ λ}{λ 2 + λ(γ x β 1 ) β 1 (γ x )} = λ(1 + z ) + (γ x β 1 z ) (2.3) IJNS for contribution: editor@nonlinearscience.org.uk
3 Dibakar Ghosh: Stability and projective synchronization in multiple 29 Substituting λ = a + ib into equation (2.3) gives D(a, b, τ) = {(α 1 + α 2 )e (a+ib)τ a ib}{(a + ib) 2 + (a + ib)(γ x β 1 ) β 1 (γ x )} Separating real and imaginary part of the critical condition D(a, b, τ) = yields, and {e aτ (α 1 + α 2 )cos(bτ) a}{a 2 b 2 + a(γ x β 1 ) β 1 (γ x )} (a + ib)(1 + z ) (γ x β 1 z ) +{e aτ (α 1 + α 2 )sin(bτ) + b}{2ab + b(γ x β 1 )} a(1 + z ) (γ x β 1 z ) = {e aτ (α 1 + α 2 )cos(bτ) a}{2ab + b(γ x β 1 )} {e aτ (α 1 + α 2 )sin(bτ) + b}{a 2 b 2 + a(γ x β 1 ) β 1 (γ x )} b(1 + z ) = According to D-subdivision method by setting a = in (2.4) and (2.5), the stability boundary are determine either by the points that yields either a root λ = or a pair of purely imaginary roots of the following equation (α 1 + α 2 ){b 2 + β 1 (γ x )}cos(bτ) b(γ x β 1 ){(α 1 + α 2 )sin(bτ) + b} + (γ x β 1 z ) = b(α 1 + α 2 )(γ x β 1 )cos(bτ) + {(α 1 + α 2 )sin(bτ) + b}{b 2 + β 1 (γ x )} b(1 + z ) = (2.6) when b =, i.e. λ = then above equation yields where Eliminating τ from (2.6) gives Let µ = b 2 and (2.4) (2.5) (γ x )(α 1 + α 2 )β 1 + γ x β 1 z = (2.7) {(γ x β 1 z ) b 2 (γ x β 1 )} 2 + {b(1 + z β 1 γ + β 1 x ) b 3 } 3 = (α 1 + α 2 ) 2 {(b 2 + β 1 (γ x )) 2 + b 2 (γ x β 1 ) 2 } (2.8) µ 3 + A 1 µ 2 + A 2 µ + A 3 = (2.9) A 1 = (x γ) 2 2(1 + z ) + β 2 1 (α 1 + α 2 ) 2 A 2 = (x γ) 2 {β 2 1 (α 1 + α 2 ) 2 2} + (1 + z ) 2 2β 2 1z β 2 1(α 1 + α 2 ) 2 A 3 = (x γ) 2 {1 (α 1 + α 2 )β 2 1} + β 2 1z 2 + 2β 1 z (x γ) In the following, we need to seek conditions under which equation (2.9) has at least one positive root. Denote h(µ) = µ 3 + A 1 µ 2 + A 2 µ + A 3 (2.1) Since h(µ) as µ, we conclude that if A 3 <, then equation (2.9) has at least one positive root. From (2.1) we have dh(µ) dµ = 3µ2 + 2A 1 µ + A 2 Clearly, if = A 2 1 3A 2, then the function h(µ) is monotone increasing in µ [, ). Thus, when A 3 and, equation (2.1) has no positive real roots. On the other hand, when A and >, the following equation 3µ 2 + 2A 1 µ + A 2 = (2.11) has two real roots µ 1 = A and µ 2 = A 1 3 (2.12) Obviously, h (µ 1 ) = 2 > and h (µ 2 ) = 2 <. It follows that µ 1 and µ 2 are the local minimum and the local maximum of h(µ), respectively. Hence, we have the following simple property. IJNS homepage:
4 21 International Journal of Nonlinear Science,Vol.7(29),No.2,pp Property 1 Suppose that A 1 and >, then linear equation of equation (2.9) has positive roots if and only if µ 1 > and h(µ 1 ). Summarizing the above discussion, we have the following simple lemma. Lemma 1 For the polynomial equation (2.9), we have the following results i) if A 3 < then equation (2.9) has at least one positive root. ii) if A 3 and = A 2 1 3A 2, then equation (2.9) has no positive roots. iii) if A 3 and = A 2 1 3A 2 >, then equation (2.9) has positive roots if and only if µ 1 = 1 3 ( A 1 + ) > and h(µ 1 ). Suppose that equation (2.9) has positive roots. Without loss of generality, we assume that it has three positive roots, defined by µ 1, µ 2 and µ 3 respectively. Then equation (2.8) has three positive roots From (2.6), we have b 1 = µ 1, b 2 = µ 2 and b 3 = µ 3 cos(bτ) = b2 (γ x β 1 )[ 1 z + 2b 2 + 2β 1 (γ x )] (b 2 + β 1 γ β 1 x )(γ x β 1 z ) (α 1 + α 2 )[{b 2 + β 1 (γ x )} 2 + b 2 (γ x β 1 ) 2 ] Thus if we denote [ [ ] ] τ (j) k = 1 b k cos 1 b 2 k (γ x β 1 ){ 1 z +2b 2 k +2β 1(γ x )} (b 2 k +β 1γ β 1 x )(γ x β 1 z ) + 2jπ (α 1 +α 2 )[{b 2 k +β 1(γ x )} 2 +b 2 k (γ x β 1 ) 2 ] (2.13) where k = 1, 2, 3; j =, 1, 2,..., then ±ib k is a pair of purely imaginary roots of equation (2.2) with τ (j) k. Define τ = τ () k = min k (1,2,3) {τ () k }, b = b k (2.14) Note that when τ 1 = τ 2 =, then equation (2.2) becomes λ 3 + B 1 λ 2 + B 2 λ + B 3 = (2.15) where B 1 = γ x β 1 α 1 α 2, B 2 = β 1 (γ x ) + (1 + z ) (α 1 + α 2 )(γ x β 1 ) and B 3 = β 1 (α 1 + α 2 )(γ x ) + (γ x β 1 z ). Therefore, applying the above results we obtain the following lemma: Lemma 2 For the third degree transcendental equation (2.2), we have i) if A 3 and = A 2 1 3A 2, then all roots with positive real parts of equation (2.2) has the same sum of those of the polynomial equation (2.15) for all τ. ii) if either A 3 < or A 3, = A 2 1 3A 2 >, µ 1 > and h(µ 1 ), then all roots with positive real parts of equation (2.2) has the same sum to those of the polynomial equation (2.15) for τ [, τ ). From equation (2.2), one may find where ( ) dλ 1 = σ 1 σ 3 dτ λ=ib k σ 2 σ 4 σ 1 = { 3b 2 k β 1(γ x )+1+z }{(γ x β 1 )b 2 k (γ x β 1 z )}+2b 2 k (γ x β 1 ){b 2 k 1 z +β 1 (γ x )} σ 2 = [(γ x β 1 )b 2 k (γ x β 1 z )] 2 +b 2 k [b2 k 1 z +β 1 (γ x )] 2 σ 3 = (γ x β 1 ) 2 +2{b 2 k +β 1(γ x )} σ 4 = (γ x β 1 ) 2 b 2 k +{b2 k +β 1(γ x )} 2 In the following, we shall investigate the stability of equilibria of system (2.1) in a theorem. Theorem 3 If the conditions of Lemma 1 and 2 hold, then the equilibrium points E 1 or E 2 is unstable for any τ and at sequence of critical values of τ given by (2.13), system (2.1) can undergo a Hopf bifurcation near these equilibrium point provided real part of ( ) dλ 1 dτ. λ=ib k IJNS for contribution: editor@nonlinearscience.org.uk
5 Dibakar Ghosh: Stability and projective synchronization in multiple (a).3 (b) x 1 (t), x 2 (t) e = x 2 (t) α x 1 (t) time time Figure 1: a) Projective synchronization between x 1 (t) and x 2 (t), (b) error dynamics of projective synchronization for α = Projective synchronization via linear observer 3.1 General formula In this section we shall use linear observer design to projective synchronization in time delay system. Consider the coupled time delay system as ẋ = f(x, x τ1 ) (3.1) ẏ = f(y, y τ1 ) + u(x, y) (3.2) where x, y R n, f : R n R n is a nonlinear vector field and u(x, y) is the control term. A definition of projective synchronization is presented below. Definition 4 Systems (3.1) and (3.2) are said to be projective synchronization if the dynamical behavior in which the amplitude of the masters state variable and that of the slave s synchronizes up to a constant scaling factor α, i.e. y αx as t. and The synchronization manifold of systems (3.1) and (3.2) is We consider the dynamic (3.1) in the form y = αx (3.3) ẋ = Ax + Bf(x) + Cg(x τ1 ) + D (3.4) We defined the response system and synchronization signal respectively as ẏ = Ay + (αz ky) + Dα (3.5) z = Bf(x) + Cg(x τ1 ) + kx (3.6) where k is the coupling strength. Then the dynamic system (3.5) is said to be linear projective observer of system (3.1) if its state y αx as t. Moreover system (3.5) is said to be global projective linear observer of (3.1) if y αx as t for any initial condition x() and y(). Let e = y αx be the projective synchronization error. Then the error dynamics is ė = ẏ αẋ = (A k)e (3.7) IJNS homepage:
6 212 International Journal of Nonlinear Science,Vol.7(29),No.2,pp (a) 1 (b) 2.8 x 1 (t), x 2 (t) time e=x 2 (t) + α x 1 (t) time Figure 2: a) anti-phase projective synchronization between x 1 (t) and x 2 (t), (b) error dynamics of anti-phase projective synchronization for α = 2.. Therefore, if the controllability matrix [k Ak A 2 k... A n 1 k] is full rank, the drive system (3.1) and the linear observer (3.5) synchronize for any scaling factor α. There are two different situation arises depending upon the sign of α. For α = 1, identical synchronization occur, whereas for α = 1, anti-phase synchronization is obtain. For α > (α 1), we get projective synchronization and for α < (α 1), one obtain anti-phase projective synchronization. The main advantage of this method is that it does not require computation of any Lyapunov exponents. In the next part we numerically check the effectiveness of the above approach. 3.2 Numerical simulation To test the effectiveness of the above approach for projective synchronization, we consider the unidirectional coupled multidelay Rössler system as x 1 = y 1 z 1 + α 1 x 1 (t τ 1 ) + α 2 x 1 (t τ 2 ) y 1 = x 1 + β 1 y 1 (3.8) z 1 = β 2 + z 1 (x 1 γ) and x 2 = y 2 z 2 + α[α 1 x 1 (t τ 1 ) + α 2 x 1 (t τ 2 )] + k(αx 1 x 2 ) y 2 = x 2 + β 1 y 2 + k(αy 1 y 2 ) (3.9) z 2 = αβ 2 γz 2 + αx 1 z 1 + k(αz 1 z 2 ) The drive system (3.8) is in chaotic state[19] for the set of parameter values α 1 =.2, α 2 =.5, β 1 = β 2 =.2, γ = 5.7, τ 1 = 1. and τ 2 = 2.. For k =.5, identical and anti-phase synchronization is obtained for α = 1 and α = 1 respectively. Figure 1(a) shows the time series of the drive system x 1 (t) (solid line) and the response system x 2 (t)(dotted line) for k =.5 and α = 2.. The time series of the error system is shown in figure 1(b). It is implied that all the state variables tend to be synchronized in a proportional relation for α = 2., i.e. x 2 (t) = 2.x 1 (t). Similarly for other relations are satisfied, i.e. y 2 (t) = 2.y 1 (t) and z 2 (t) = 2.z 1 (t). The time series of the drive system x 1 (t) (solid line) and the response system x 2 (t)(dotted line) for k =.5 and α = 2. are shown in Figure 2(a). The time series of the error system is shown in figure 2(b). It is shown from figure 2(a) that the difference of phase angles of the synchronized trajectories is π, i.e. anti-phase pattern. Relation between drive and response systems is x 2 (t) = 2.x 1 (t). In figure 3(a), the chaotic attractor of drive system (3.8) is reported. For α = 2., projective synchronization occurs and the attractor of the response system (3.9) has been scaled by twice than that the attractor IJNS for contribution: editor@nonlinearscience.org.uk
7 Dibakar Ghosh: Stability and projective synchronization in multiple (a) (b) (c) y y 2 1 y x x x 2 5 Figure 3: a) Chaotic attractors of a) drive system (3.8) and response system (3.9) for (b) α = 2. and (c) α = 2.. of drive system (3.8) (figure 3(b)), synchronized chaotic attractors with an identical phase pattern where the phase angle between the synchronized trajectories is zero. Anti-phase projective synchronization with twice scale for α = 2. is shown in figure 3(c). From this figure it is observed that the synchronized chaotic attractors are in anti-phase pattern and the phase angle between the synchronized trajectories is π. Similar results are obtained for other values of scaling factor α. 4 Conclusions Chaos phenomena exist in multiple time delay Rössler system. A new technique of projective synchronization for a class of multiple time delay systems via linear observer has been developed. The proposed approach can be successfully applied to several well-known time delay systems and it does not require computation of any Lyapunov exponent. This projective synchronization in multiple time delay system are very much applicable in cryptography for fast communication. References [1] Sparrow C : Bifurcation in the Lorenz equation: Lecture notes in Applied Mathematics. (Springer- Verlag)(1982) [2] Sun Z, Xu W, Yang X and Fang T : Effects of time delays on bifurcation and chaos in a non-autonomous system with multiple time delays. Chaos, Solitons and Fractals. 31: 39-53(27) [3] Pecora L M and Carroll T L : Synchronization in chaotic systems. Phys. Rev. Lett. 64: (199) [4] CHAOS, Special issue on chaos synchronization 7,N4 (1997) edited by Ditto W L and Showalter K, Chen G and Dong X : From Chaos to Order.Methodologies, Perspectives and Applications (World Scientific, Singapore,1998), Handbook of Chaos Control, Ed. Schuster H G (Wiley-VCH, Weinheim,1999) [5] Fujisaka H and Yamada T : Stability Theory of Synchronized Motion in Coupled-Oscillator Systems. Prog. Theor. Phys. 69(1), 32-47(1983), Ghosh D and Roy Chowdhury A : Various Types of Chaos Synchronization- a Comparative Study of Empirical Mode Decomposition and Wavelet Approach. Int. J. Nonlinear Sci. 4(1): 52-66(27) [6] Ghosh D, Ray D and Roy Chowdhury A : Generalized and phase synchronization between two different time-delayed systems Mod. Phys. Letts. B (Accepted 28), Shahverdiev E M and Shore K A : Generalized synchronization in time-delayed systems. Phys. Rev. E 71:1621(25) IJNS homepage:
8 214 International Journal of Nonlinear Science,Vol.7(29),No.2,pp [7] Rosenblum M G, Pikovsky A S and Kurths J : Phase Synchronization of Chaotic Oscillators. Phys. Rev. Lett. 76: (1996), Yalcinkaya T and Lai Y C : Phase Characterization of Chaos. Phys. Rev. Lett. 79: (1997), Senthilkumar D V, Lakshmanan M and Kurths J : Phase synchronization in time-delay systems. Phys. Rev. E. 74: 3525(R)(26) [8] Zhan M, Wei G W and Lai C H : Transition from intermittency to periodicity in lag synchronization in coupled Rössler oscillators. Phys. Rev. E. 65:3622-5(22) [9] Voss H U : Dynamic Long-Term Anticipation of Chaotic States. Phys. Rev. Lett. 87: 1412(21) [1] Cao L Y and Lai Y C : Antiphase synchronism in chaotic systems. Phys. Rev. E. 58: (1998) [11] Banerjee S, Ghosh D and Roy Chowdhury A : Multiplexing synchronization and its applications in cryptography. Physica Scripta. 78, (28) [12] Mainieri R and Rehacek J : Projective Synchronization In Three-Dimensional Chaotic Systems. Phys. Rev. Lett. 82: (1999) [13] Chee C Y and Xu D : Control of the formation of projective synchronisation in lower-dimensional discrete-time systems. Phys. Lett. A. 318: (23) [14] Li G H, Zhou S P and Yang K : Generalized projective synchronization between two different chaotic systems using active backstepping control. Phys. Lett. A. 355:326-33(26) [15] Grassi G and Miller D A : Projective synchronization via a linear observer : application to time-delay, continuous-time and discrete-time systems. Int. J. Bifur. Chaos. 17(4): (27) [16] Grassi G and Mascolo S : Nonlinear observer design to synchronize hyperchaotic systems via scalar signal. IEEE, Transction on Circuits and systems-1: Fundamental theory and applications. 44: (1997) [17] Ghosh D, Banerjee S and Roy Chowdhury A : Synchronization between variable time delayed systems and cryptography. Europhysics Letters. 8: 36(27) [18] Banerjee S, Ghosh D, Ray A and Roy Chowdhury A : Synchronization between two different time delayed systems and image encryption. Europhysics Letters. 81:26(28) [19] Ghosh D, Roy Chowdhury A and Saha P : Multiple delay Rössler system-bifurcation and chaos control. Chaos, Solitons and Fractals. 35: (28) [2] Rössler O E : An equation for continuous chaos. Phys. Lett. A. 57: (1976) IJNS for contribution: editor@nonlinearscience.org.uk
Generalized-Type Synchronization of Hyperchaotic Oscillators Using a Vector Signal
Commun. Theor. Phys. (Beijing, China) 44 (25) pp. 72 78 c International Acaemic Publishers Vol. 44, No. 1, July 15, 25 Generalize-Type Synchronization of Hyperchaotic Oscillators Using a Vector Signal
More informationFunction Projective Synchronization of Discrete-Time Chaotic and Hyperchaotic Systems Using Backstepping Method
Commun. Theor. Phys. (Beijing, China) 50 (2008) pp. 111 116 c Chinese Physical Society Vol. 50, No. 1, July 15, 2008 Function Projective Synchronization of Discrete-Time Chaotic and Hyperchaotic Systems
More informationGeneralized projective synchronization of a class of chaotic (hyperchaotic) systems with uncertain parameters
Vol 16 No 5, May 2007 c 2007 Chin. Phys. Soc. 1009-1963/2007/16(05)/1246-06 Chinese Physics and IOP Publishing Ltd Generalized projective synchronization of a class of chaotic (hyperchaotic) systems with
More informationBidirectional Partial Generalized Synchronization in Chaotic and Hyperchaotic Systems via a New Scheme
Commun. Theor. Phys. (Beijing, China) 45 (2006) pp. 1049 1056 c International Academic Publishers Vol. 45, No. 6, June 15, 2006 Bidirectional Partial Generalized Synchronization in Chaotic and Hyperchaotic
More informationComplete Synchronization, Anti-synchronization and Hybrid Synchronization Between Two Different 4D Nonlinear Dynamical Systems
Mathematics Letters 2016; 2(5): 36-41 http://www.sciencepublishinggroup.com/j/ml doi: 10.11648/j.ml.20160205.12 Complete Synchronization, Anti-synchronization and Hybrid Synchronization Between Two Different
More informationCharacteristics and synchronization of time-delay systems driven by a common noise
Eur. Phys. J. Special Topics 87, 87 93 (2) c EDP Sciences, Springer-Verlag 2 DOI:.4/epjst/e2-273-4 THE EUROPEAN PHYSICAL JOURNAL SPECIAL TOPICS Regular Article Characteristics and synchronization of time-delay
More informationThe Application of Contraction Theory in Synchronization of Coupled Chen Systems
ISSN 1749-3889 (print), 1749-3897 (online) International Journal of Nonlinear Science Vol.9(2010) No.1,pp.72-77 The Application of Contraction Theory in Synchronization of Coupled Chen Systems Hongxing
More informationControlling the Period-Doubling Bifurcation of Logistic Model
ISSN 1749-3889 (print), 1749-3897 (online) International Journal of Nonlinear Science Vol.20(2015) No.3,pp.174-178 Controlling the Period-Doubling Bifurcation of Logistic Model Zhiqian Wang 1, Jiashi Tang
More informationChaos synchronization of complex Rössler system
Appl. Math. Inf. Sci. 7, No. 4, 1415-1420 (2013) 1415 Applied Mathematics & Information Sciences An International Journal http://dx.doi.org/10.12785/amis/070420 Chaos synchronization of complex Rössler
More informationStudy on Proportional Synchronization of Hyperchaotic Circuit System
Commun. Theor. Phys. (Beijing, China) 43 (25) pp. 671 676 c International Academic Publishers Vol. 43, No. 4, April 15, 25 Study on Proportional Synchronization of Hyperchaotic Circuit System JIANG De-Ping,
More informationPhase Synchronization of Van der Pol-Duffing Oscillators Using Decomposition Method
Adv. Studies Theor. Phys., Vol. 3, 29, no. 11, 429-437 Phase Synchronization of Van der Pol-Duffing Oscillators Using Decomposition Method Gh. Asadi Cordshooli Department of Physics, Shahr-e-Rey Branch,
More informationAnti-synchronization of a new hyperchaotic system via small-gain theorem
Anti-synchronization of a new hyperchaotic system via small-gain theorem Xiao Jian( ) College of Mathematics and Statistics, Chongqing University, Chongqing 400044, China (Received 8 February 2010; revised
More informationA Generalized Anti-synchronization of Discrete Chaotic Maps via Linear Transformations
ISSN 749-3889 (print), 749-3897 (online) International Journal of Nonlinear Science Vol.24(27) No., pp.44-52 A Generalized Anti-synchronization of Discrete Chaotic Maps via Linear Transformations Debjani
More informationGLOBAL CHAOS SYNCHRONIZATION OF HYPERCHAOTIC QI AND HYPERCHAOTIC JHA SYSTEMS BY ACTIVE NONLINEAR CONTROL
GLOBAL CHAOS SYNCHRONIZATION OF HYPERCHAOTIC QI AND HYPERCHAOTIC JHA SYSTEMS BY ACTIVE NONLINEAR CONTROL Sundarapandian Vaidyanathan 1 1 Research and Development Centre, Vel Tech Dr. RR & Dr. SR Technical
More information3. Controlling the time delay hyper chaotic Lorenz system via back stepping control
ISSN 1746-7659, England, UK Journal of Information and Computing Science Vol 10, No 2, 2015, pp 148-153 Chaos control of hyper chaotic delay Lorenz system via back stepping method Hanping Chen 1 Xuerong
More informationSynchronizing Chaotic Systems Based on Tridiagonal Structure
Proceedings of the 7th World Congress The International Federation of Automatic Control Seoul, Korea, July 6-, 008 Synchronizing Chaotic Systems Based on Tridiagonal Structure Bin Liu, Min Jiang Zengke
More informationComputers and Mathematics with Applications. Adaptive anti-synchronization of chaotic systems with fully unknown parameters
Computers and Mathematics with Applications 59 (21) 3234 3244 Contents lists available at ScienceDirect Computers and Mathematics with Applications journal homepage: www.elsevier.com/locate/camwa Adaptive
More informationComplete synchronization and generalized synchronization of one-way coupled time-delay systems
Complete synchronization and generalized synchronization of one-way coupled time-delay systems Meng Zhan, 1 Xingang Wang, 1 Xiaofeng Gong, 1 G. W. Wei,,3 and C.-H. Lai 4 1 Temasek Laboratories, National
More informationHYBRID CHAOS SYNCHRONIZATION OF HYPERCHAOTIC LIU AND HYPERCHAOTIC CHEN SYSTEMS BY ACTIVE NONLINEAR CONTROL
HYBRID CHAOS SYNCHRONIZATION OF HYPERCHAOTIC LIU AND HYPERCHAOTIC CHEN SYSTEMS BY ACTIVE NONLINEAR CONTROL Sundarapandian Vaidyanathan 1 1 Research and Development Centre, Vel Tech Dr. RR & Dr. SR Technical
More informationADAPTIVE CONTROL AND SYNCHRONIZATION OF HYPERCHAOTIC NEWTON-LEIPNIK SYSTEM
ADAPTIVE CONTROL AND SYNCHRONIZATION OF HYPERCHAOTIC NEWTON-LEIPNIK SYSTEM Sundarapandian Vaidyanathan 1 1 Research and Development Centre, Vel Tech Dr. RR & Dr. SR Technical University Avadi, Chennai-600
More informationA New Modified Hyperchaotic Finance System and its Control
ISSN 1749-3889 (print), 1749-3897 (online) International Journal of Nonlinear Science Vol.8(2009) No.1,pp.59-66 A New Modified Hyperchaotic Finance System and its Control Juan Ding, Weiguo Yang, Hongxing
More informationHomotopy Perturbation Method for the Fisher s Equation and Its Generalized
ISSN 749-889 (print), 749-897 (online) International Journal of Nonlinear Science Vol.8(2009) No.4,pp.448-455 Homotopy Perturbation Method for the Fisher s Equation and Its Generalized M. Matinfar,M. Ghanbari
More informationADAPTIVE CHAOS SYNCHRONIZATION OF UNCERTAIN HYPERCHAOTIC LORENZ AND HYPERCHAOTIC LÜ SYSTEMS
ADAPTIVE CHAOS SYNCHRONIZATION OF UNCERTAIN HYPERCHAOTIC LORENZ AND HYPERCHAOTIC LÜ SYSTEMS Sundarapandian Vaidyanathan 1 1 Research and Development Centre, Vel Tech Dr. RR & Dr. SR Technical University
More informationLag anti-synchronization of delay coupled chaotic systems via a scalar signal
Lag anti-synchronization of delay coupled chaotic systems via a scalar signal Mohammad Ali Khan Abstract. In this letter, a chaotic anti-synchronization (AS scheme is proposed based on combining a nonlinear
More informationHopf Bifurcation and Limit Cycle Analysis of the Rikitake System
ISSN 749-3889 (print), 749-3897 (online) International Journal of Nonlinear Science Vol.4(0) No.,pp.-5 Hopf Bifurcation and Limit Cycle Analysis of the Rikitake System Xuedi Wang, Tianyu Yang, Wei Xu Nonlinear
More informationAdaptive feedback synchronization of a unified chaotic system
Physics Letters A 39 (4) 37 333 www.elsevier.com/locate/pla Adaptive feedback synchronization of a unified chaotic system Junan Lu a, Xiaoqun Wu a, Xiuping Han a, Jinhu Lü b, a School of Mathematics and
More informationNumerical Simulation of the Generalized Hirota-Satsuma Coupled KdV Equations by Variational Iteration Method
ISSN 1749-3889 (print), 1749-3897 (online) International Journal of Nonlinear Science Vol.7(29) No.1,pp.67-74 Numerical Simulation of the Generalized Hirota-Satsuma Coupled KdV Equations by Variational
More informationDR. DIBAKAR GHOSH. Assistant Professor. Physics and Applied Mathematics Unit. Indian Statistical Institute
DR. DIBAKAR GHOSH Assistant Professor Physics and Applied Mathematics Unit Indian Statistical Institute 203 B. T. Road, Kolkata 700108, India. Mobile: +91-9830334136 E-Mail: diba.ghosh@gmail.com dibakar@isical.ac.in
More informationDynamical Behavior And Synchronization Of Chaotic Chemical Reactors Model
Iranian Journal of Mathematical Chemistry, Vol. 6, No. 1, March 2015, pp. 81 92 IJMC Dynamical Behavior And Synchronization Of Chaotic Chemical Reactors Model HOSSEIN KHEIRI 1 AND BASHIR NADERI 2 1 Faculty
More informationGLOBAL CHAOS SYNCHRONIZATION OF UNCERTAIN SPROTT J AND K SYSTEMS BY ADAPTIVE CONTROL
GLOBAL CHAOS SYNCHRONIZATION OF UNCERTAIN SPROTT J AND K SYSTEMS BY ADAPTIVE CONTROL Sundarapandian Vaidyanathan 1 1 Research and Development Centre, Vel Tech Dr. RR & Dr. SR Technical University Avadi,
More informationFunction Projective Synchronization of Fractional-Order Hyperchaotic System Based on Open-Plus-Closed-Looping
Commun. Theor. Phys. 55 (2011) 617 621 Vol. 55, No. 4, April 15, 2011 Function Projective Synchronization of Fractional-Order Hyperchaotic System Based on Open-Plus-Closed-Looping WANG Xing-Yuan ( ), LIU
More informationADAPTIVE DESIGN OF CONTROLLER AND SYNCHRONIZER FOR LU-XIAO CHAOTIC SYSTEM
ADAPTIVE DESIGN OF CONTROLLER AND SYNCHRONIZER FOR LU-XIAO CHAOTIC SYSTEM WITH UNKNOWN PARAMETERS Sundarapandian Vaidyanathan 1 1 Research and Development Centre, Vel Tech Dr. RR & Dr. SR Technical University
More informationGenerating a Complex Form of Chaotic Pan System and its Behavior
Appl. Math. Inf. Sci. 9, No. 5, 2553-2557 (2015) 2553 Applied Mathematics & Information Sciences An International Journal http://dx.doi.org/10.12785/amis/090540 Generating a Complex Form of Chaotic Pan
More informationTime-delay feedback control in a delayed dynamical chaos system and its applications
Time-delay feedback control in a delayed dynamical chaos system and its applications Ye Zhi-Yong( ), Yang Guang( ), and Deng Cun-Bing( ) School of Mathematics and Physics, Chongqing University of Technology,
More informationKingSaudBinAbdulazizUniversityforHealthScience,Riyadh11481,SaudiArabia. Correspondence should be addressed to Raghib Abu-Saris;
Chaos Volume 26, Article ID 49252, 7 pages http://dx.doi.org/.55/26/49252 Research Article On Matrix Projective Synchronization and Inverse Matrix Projective Synchronization for Different and Identical
More informationA SYSTEMATIC PROCEDURE FOR SYNCHRONIZING HYPERCHAOS VIA OBSERVER DESIGN
Journal of Circuits, Systems, and Computers, Vol. 11, No. 1 (22) 1 16 c World Scientific Publishing Company A SYSTEMATIC PROCEDURE FOR SYNCHRONIZING HYPERCHAOS VIA OBSERVER DESIGN GIUSEPPE GRASSI Dipartimento
More informationFinite-time hybrid synchronization of time-delay hyperchaotic Lorenz system
ISSN 1746-7659 England UK Journal of Information and Computing Science Vol. 10 No. 4 2015 pp. 265-270 Finite-time hybrid synchronization of time-delay hyperchaotic Lorenz system Haijuan Chen 1 * Rui Chen
More informationCONTROLLING CHAOTIC DYNAMICS USING BACKSTEPPING DESIGN WITH APPLICATION TO THE LORENZ SYSTEM AND CHUA S CIRCUIT
Letters International Journal of Bifurcation and Chaos, Vol. 9, No. 7 (1999) 1425 1434 c World Scientific Publishing Company CONTROLLING CHAOTIC DYNAMICS USING BACKSTEPPING DESIGN WITH APPLICATION TO THE
More informationADAPTIVE SYNCHRONIZATION FOR RÖSSLER AND CHUA S CIRCUIT SYSTEMS
Letters International Journal of Bifurcation and Chaos, Vol. 12, No. 7 (2002) 1579 1597 c World Scientific Publishing Company ADAPTIVE SYNCHRONIZATION FOR RÖSSLER AND CHUA S CIRCUIT SYSTEMS A. S. HEGAZI,H.N.AGIZA
More informationTHE ACTIVE CONTROLLER DESIGN FOR ACHIEVING GENERALIZED PROJECTIVE SYNCHRONIZATION OF HYPERCHAOTIC LÜ AND HYPERCHAOTIC CAI SYSTEMS
THE ACTIVE CONTROLLER DESIGN FOR ACHIEVING GENERALIZED PROJECTIVE SYNCHRONIZATION OF HYPERCHAOTIC LÜ AND HYPERCHAOTIC CAI SYSTEMS Sarasu Pakiriswamy 1 and Sundarapandian Vaidyanathan 1 1 Department of
More informationADAPTIVE CONTROL AND SYNCHRONIZATION OF A GENERALIZED LOTKA-VOLTERRA SYSTEM
ADAPTIVE CONTROL AND SYNCHRONIZATION OF A GENERALIZED LOTKA-VOLTERRA SYSTEM Sundarapandian Vaidyanathan 1 1 Research and Development Centre, Vel Tech Dr. RR & Dr. SR Technical University Avadi, Chennai-600
More informationA Generalization of Some Lag Synchronization of System with Parabolic Partial Differential Equation
American Journal of Theoretical and Applied Statistics 2017; 6(5-1): 8-12 http://www.sciencepublishinggroup.com/j/ajtas doi: 10.11648/j.ajtas.s.2017060501.12 ISSN: 2326-8999 (Print); ISSN: 2326-9006 (Online)
More informationK. Pyragas* Semiconductor Physics Institute, LT-2600 Vilnius, Lithuania Received 19 March 1998
PHYSICAL REVIEW E VOLUME 58, NUMBER 3 SEPTEMBER 998 Synchronization of coupled time-delay systems: Analytical estimations K. Pyragas* Semiconductor Physics Institute, LT-26 Vilnius, Lithuania Received
More informationA Novel Three Dimension Autonomous Chaotic System with a Quadratic Exponential Nonlinear Term
ETASR - Engineering, Technology & Applied Science Research Vol., o.,, 9-5 9 A Novel Three Dimension Autonomous Chaotic System with a Quadratic Exponential Nonlinear Term Fei Yu College of Information Science
More informationElectronic Circuit Simulation of the Lorenz Model With General Circulation
International Journal of Physics, 2014, Vol. 2, No. 5, 124-128 Available online at http://pubs.sciepub.com/ijp/2/5/1 Science and Education Publishing DOI:10.12691/ijp-2-5-1 Electronic Circuit Simulation
More informationADAPTIVE STABILIZATION AND SYNCHRONIZATION OF HYPERCHAOTIC QI SYSTEM
ADAPTIVE STABILIZATION AND SYNCHRONIZATION OF HYPERCHAOTIC QI SYSTEM Sundarapandian Vaidyanathan 1 1 Research and Development Centre, Vel Tech Dr. RR Dr. SR Technical University Avadi, Chennai-600 062,
More informationMULTISTABILITY IN A BUTTERFLY FLOW
International Journal of Bifurcation and Chaos, Vol. 23, No. 12 (2013) 1350199 (10 pages) c World Scientific Publishing Company DOI: 10.1142/S021812741350199X MULTISTABILITY IN A BUTTERFLY FLOW CHUNBIAO
More informationNew communication schemes based on adaptive synchronization
CHAOS 17, 0114 2007 New communication schemes based on adaptive synchronization Wenwu Yu a Department of Mathematics, Southeast University, Nanjing 210096, China, Department of Electrical Engineering,
More informationarxiv:nlin/ v1 [nlin.cd] 4 Oct 2005
Synchronization of Coupled Chaotic Dynamics on Networks R. E. Amritkar and Sarika Jalan Physical Research Laboratory, Navrangpura, Ahmedabad 380 009, India. arxiv:nlin/0510008v1 [nlin.cd] 4 Oct 2005 Abstract
More informationA Novel Hyperchaotic System and Its Control
1371371371371378 Journal of Uncertain Systems Vol.3, No., pp.137-144, 009 Online at: www.jus.org.uk A Novel Hyperchaotic System and Its Control Jiang Xu, Gouliang Cai, Song Zheng School of Mathematics
More informationTracking the State of the Hindmarsh-Rose Neuron by Using the Coullet Chaotic System Based on a Single Input
ISSN 1746-7659, England, UK Journal of Information and Computing Science Vol. 11, No., 016, pp.083-09 Tracking the State of the Hindmarsh-Rose Neuron by Using the Coullet Chaotic System Based on a Single
More informationSIMPLE CHAOTIC FLOWS WITH ONE STABLE EQUILIBRIUM
International Journal of Bifurcation and Chaos, Vol. 23, No. 11 (2013) 1350188 (7 pages) c World Scientific Publishing Company DOI: 10.1142/S0218127413501885 SIMPLE CHAOTIC FLOWS WITH ONE STABLE EQUILIBRIUM
More informationA New Dynamic Phenomenon in Nonlinear Circuits: State-Space Analysis of Chaotic Beats
A New Dynamic Phenomenon in Nonlinear Circuits: State-Space Analysis of Chaotic Beats DONATO CAFAGNA, GIUSEPPE GRASSI Diparnto Ingegneria Innovazione Università di Lecce via Monteroni, 73 Lecce ITALY giuseppe.grassi}@unile.it
More informationPhase Desynchronization as a Mechanism for Transitions to High-Dimensional Chaos
Commun. Theor. Phys. (Beijing, China) 35 (2001) pp. 682 688 c International Academic Publishers Vol. 35, No. 6, June 15, 2001 Phase Desynchronization as a Mechanism for Transitions to High-Dimensional
More informationBifurcation control and chaos in a linear impulsive system
Vol 8 No 2, December 2009 c 2009 Chin. Phys. Soc. 674-056/2009/82)/5235-07 Chinese Physics B and IOP Publishing Ltd Bifurcation control and chaos in a linear impulsive system Jiang Gui-Rong 蒋贵荣 ) a)b),
More informationarxiv:nlin/ v1 [nlin.cd] 25 Apr 2001
Anticipated synchronization in coupled chaotic maps with delays arxiv:nlin/0104061v1 [nlin.cd] 25 Apr 2001 Cristina Masoller a, Damián H. Zanette b a Instituto de Física, Facultad de Ciencias, Universidad
More informationA New Circuit for Generating Chaos and Complexity: Analysis of the Beats Phenomenon
A New Circuit for Generating Chaos and Complexity: Analysis of the Beats Phenomenon DONATO CAFAGNA, GIUSEPPE GRASSI Diparnto Ingegneria Innovazione Università di Lecce via Monteroni, 73 Lecce ITALY Abstract:
More informationCONTROLLING IN BETWEEN THE LORENZ AND THE CHEN SYSTEMS
International Journal of Bifurcation and Chaos, Vol. 12, No. 6 (22) 1417 1422 c World Scientific Publishing Company CONTROLLING IN BETWEEN THE LORENZ AND THE CHEN SYSTEMS JINHU LÜ Institute of Systems
More informationA new four-dimensional chaotic system
Chin. Phys. B Vol. 19 No. 12 2010) 120510 A new four-imensional chaotic system Chen Yong ) a)b) an Yang Yun-Qing ) a) a) Shanghai Key Laboratory of Trustworthy Computing East China Normal University Shanghai
More informationInverse optimal control of hyperchaotic finance system
ISSN 1 746-7233, England, UK World Journal of Modelling and Simulation Vol. 10 (2014) No. 2, pp. 83-91 Inverse optimal control of hyperchaotic finance system Changzhong Chen 1,3, Tao Fan 1,3, Bangrong
More informationADAPTIVE CHAOS CONTROL AND SYNCHRONIZATION OF HYPERCHAOTIC LIU SYSTEM
International Journal o Computer Science, Engineering and Inormation Technology (IJCSEIT), Vol.1, No., June 011 ADAPTIVE CHAOS CONTROL AND SYNCHRONIZATION OF HYPERCHAOTIC LIU SYSTEM Sundarapandian Vaidyanathan
More informationStability and hybrid synchronization of a time-delay financial hyperchaotic system
ISSN 76-7659 England UK Journal of Information and Computing Science Vol. No. 5 pp. 89-98 Stability and hybrid synchronization of a time-delay financial hyperchaotic system Lingling Zhang Guoliang Cai
More informationChaos Synchronization of Nonlinear Bloch Equations Based on Input-to-State Stable Control
Commun. Theor. Phys. (Beijing, China) 53 (2010) pp. 308 312 c Chinese Physical Society and IOP Publishing Ltd Vol. 53, No. 2, February 15, 2010 Chaos Synchronization of Nonlinear Bloch Equations Based
More informationGeneralized function projective synchronization of chaotic systems for secure communication
RESEARCH Open Access Generalized function projective synchronization of chaotic systems for secure communication Xiaohui Xu Abstract By using the generalized function projective synchronization (GFPS)
More informationDESYNCHRONIZATION TRANSITIONS IN RINGS OF COUPLED CHAOTIC OSCILLATORS
Letters International Journal of Bifurcation and Chaos, Vol. 8, No. 8 (1998) 1733 1738 c World Scientific Publishing Company DESYNCHRONIZATION TRANSITIONS IN RINGS OF COUPLED CHAOTIC OSCILLATORS I. P.
More informationSimple approach to the creation of a strange nonchaotic attractor in any chaotic system
PHYSICAL REVIEW E VOLUME 59, NUMBER 5 MAY 1999 Simple approach to the creation of a strange nonchaotic attractor in any chaotic system J. W. Shuai 1, * and K. W. Wong 2, 1 Department of Biomedical Engineering,
More informationControlling a Novel Chaotic Attractor using Linear Feedback
ISSN 746-7659, England, UK Journal of Information and Computing Science Vol 5, No,, pp 7-4 Controlling a Novel Chaotic Attractor using Linear Feedback Lin Pan,, Daoyun Xu 3, and Wuneng Zhou College of
More informationExperimental and numerical realization of higher order autonomous Van der Pol-Duffing oscillator
Indian Journal of Pure & Applied Physics Vol. 47, November 2009, pp. 823-827 Experimental and numerical realization of higher order autonomous Van der Pol-Duffing oscillator V Balachandran, * & G Kandiban
More informationResearch Article Hopf Bifurcation Analysis and Anticontrol of Hopf Circles of the Rössler-Like System
Abstract and Applied Analysis Volume, Article ID 3487, 6 pages doi:.55//3487 Research Article Hopf Bifurcation Analysis and Anticontrol of Hopf Circles of the Rössler-Like System Ranchao Wu and Xiang Li
More informationImpulsive synchronization of chaotic systems
CHAOS 15, 023104 2005 Impulsive synchronization of chaotic systems Chuandong Li a and Xiaofeng Liao College of Computer Science and Engineering, Chongqing University, 400030 China Xingyou Zhang College
More informationADAPTIVE CONTROLLER DESIGN FOR THE ANTI-SYNCHRONIZATION OF HYPERCHAOTIC YANG AND HYPERCHAOTIC PANG SYSTEMS
ADAPTIVE CONTROLLER DESIGN FOR THE ANTI-SYNCHRONIZATION OF HYPERCHAOTIC YANG AND HYPERCHAOTIC PANG SYSTEMS Sundarapandian Vaidyanathan 1 1 Research and Development Centre, Vel Tech Dr. RR & Dr. SR Technical
More informationRecent new examples of hidden attractors
Eur. Phys. J. Special Topics 224, 1469 1476 (2015) EDP Sciences, Springer-Verlag 2015 DOI: 10.1140/epjst/e2015-02472-1 THE EUROPEAN PHYSICAL JOURNAL SPECIAL TOPICS Review Recent new examples of hidden
More informationPhase Synchronization of Coupled Rossler Oscillators: Amplitude Effect
Commun. Theor. Phys. (Beijing, China) 47 (2007) pp. 265 269 c International Academic Publishers Vol. 47, No. 2, February 15, 2007 Phase Synchronization of Coupled Rossler Oscillators: Amplitude Effect
More information698 Zou Yan-Li et al Vol. 14 and L 2, respectively, V 0 is the forward voltage drop across the diode, and H(u) is the Heaviside function 8 < 0 u < 0;
Vol 14 No 4, April 2005 cfl 2005 Chin. Phys. Soc. 1009-1963/2005/14(04)/0697-06 Chinese Physics and IOP Publishing Ltd Chaotic coupling synchronization of hyperchaotic oscillators * Zou Yan-Li( ΠΛ) a)y,
More informationConstruction of a New Fractional Chaotic System and Generalized Synchronization
Commun. Theor. Phys. (Beijing, China) 5 (2010) pp. 1105 1110 c Chinese Physical Society and IOP Publishing Ltd Vol. 5, No. 6, June 15, 2010 Construction of a New Fractional Chaotic System and Generalized
More informationDynamical analysis and circuit simulation of a new three-dimensional chaotic system
Dynamical analysis and circuit simulation of a new three-dimensional chaotic system Wang Ai-Yuan( 王爱元 ) a)b) and Ling Zhi-Hao( 凌志浩 ) a) a) Department of Automation, East China University of Science and
More informationGLOBAL CHAOS SYNCHRONIZATION OF UNCERTAIN LORENZ-STENFLO AND QI 4-D CHAOTIC SYSTEMS BY ADAPTIVE CONTROL
GLOBAL CHAOS SYNCHRONIZATION OF UNCERTAIN LORENZ-STENFLO AND QI 4-D CHAOTIC SYSTEMS BY ADAPTIVE CONTROL Sundarapandian Vaidyanathan 1 1 Research and Development Centre, Vel Tech Dr. RR & Dr. SR Technical
More informationHopf Bifurcation of a Nonlinear System Derived from Lorenz System Using Centre Manifold Approach ABSTRACT. 1. Introduction
Malaysian Journal of Mathematical Sciences 10(S) March : 1-13 (2016) Special Issue: The 10th IMT-GT International Conference on Mathematics, Statistics and its Applications 2014 (ICMSA 2014) MALAYSIAN
More informationThe projects listed on the following pages are suitable for MSc/MSci or PhD students. An MSc/MSci project normally requires a review of the
The projects listed on the following pages are suitable for MSc/MSci or PhD students. An MSc/MSci project normally requires a review of the literature and finding recent related results in the existing
More informationImage encryption based on the tracking control Hindmarsh-Rose system via Genesio-Tesi system
ISSN 1746-7659, England, UK Journal of Information and Computing Science Vol. 1, No., 017, pp.13-19 Image encryption based on the tracking control Hindmarsh-Rose system via Genesio-Tesi system Keming Tang
More informationSecure Communications Based on the. Synchronization of the New Lorenz-like. Attractor Circuit
Advanced Studies in Theoretical Physics Vol. 9, 15, no. 8, 379-39 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/1.1988/astp.15.58 Secure Communications Based on the Synchronization of the New Lorenz-like
More informationSome explicit formulas of Lyapunov exponents for 3D quadratic mappings
Some explicit formulas of Lyapunov exponents for 3D quadratic mappings Zeraoulia Elhadj 1,J.C.Sprott 2 1 Department of Mathematics, University of Tébessa, (12002), Algeria. E-mail: zeraoulia@mail.univ-tebessa.dz
More informationA Unified Lorenz-Like System and Its Tracking Control
Commun. Theor. Phys. 63 (2015) 317 324 Vol. 63, No. 3, March 1, 2015 A Unified Lorenz-Like System and Its Tracking Control LI Chun-Lai ( ) 1, and ZHAO Yi-Bo ( ) 2,3 1 College of Physics and Electronics,
More informationRobust Gain Scheduling Synchronization Method for Quadratic Chaotic Systems With Channel Time Delay Yu Liang and Horacio J.
604 IEEE TRANSACTIONS ON CIRCUITS AND SYSTEMS I: REGULAR PAPERS, VOL. 56, NO. 3, MARCH 2009 Robust Gain Scheduling Synchronization Method for Quadratic Chaotic Systems With Channel Time Delay Yu Liang
More informationSecure Communication Using H Chaotic Synchronization and International Data Encryption Algorithm
Secure Communication Using H Chaotic Synchronization and International Data Encryption Algorithm Gwo-Ruey Yu Department of Electrical Engineering I-Shou University aohsiung County 840, Taiwan gwoyu@isu.edu.tw
More informationarxiv: v1 [eess.sp] 4 Dec 2017
DINCON 2017 CONFERÊNCIA BRASILEIRA DE DINÂMICA, CONTROLE E APLICAÇÕES 30 de outubro a 01 de novembro de 2017 São José do Rio Preto/SP Synchronization on the accuracy of chaotic oscillators simulations
More informationSynchronization of identical new chaotic flows via sliding mode controller and linear control
Synchronization of identical new chaotic flows via sliding mode controller and linear control Atefeh Saedian, Hassan Zarabadipour Department of Electrical Engineering IKI University Iran a.saedian@gmail.com,
More informationHyperchaos and hyperchaos control of the sinusoidally forced simplified Lorenz system
Nonlinear Dyn (2012) 69:1383 1391 DOI 10.1007/s11071-012-0354-x ORIGINAL PAPER Hyperchaos and hyperchaos control of the sinusoidally forced simplified Lorenz system Keihui Sun Xuan Liu Congxu Zhu J.C.
More informationCompacton Solutions and Peakon Solutions for a Coupled Nonlinear Wave Equation
ISSN 1749-3889 (print), 1749-3897 (online) International Journal of Nonlinear Science Vol 4(007) No1,pp31-36 Compacton Solutions Peakon Solutions for a Coupled Nonlinear Wave Equation Dianchen Lu, Guangjuan
More informationTHE SYNCHRONIZATION OF TWO CHAOTIC MODELS OF CHEMICAL REACTIONS
ROMAI J., v.10, no.1(2014), 137 145 THE SYNCHRONIZATION OF TWO CHAOTIC MODELS OF CHEMICAL REACTIONS Servilia Oancea 1, Andrei-Victor Oancea 2, Ioan Grosu 3 1 U.S.A.M.V., Iaşi, Romania 2 Erasmus Mundus
More informationChaos Control for the Lorenz System
Advanced Studies in Theoretical Physics Vol. 12, 2018, no. 4, 181-188 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/astp.2018.8413 Chaos Control for the Lorenz System Pedro Pablo Cárdenas Alzate
More informationADAPTIVE FEEDBACK LINEARIZING CONTROL OF CHUA S CIRCUIT
International Journal of Bifurcation and Chaos, Vol. 12, No. 7 (2002) 1599 1604 c World Scientific Publishing Company ADAPTIVE FEEDBACK LINEARIZING CONTROL OF CHUA S CIRCUIT KEVIN BARONE and SAHJENDRA
More informationGLOBAL CHAOS SYNCHRONIZATION OF PAN AND LÜ CHAOTIC SYSTEMS VIA ADAPTIVE CONTROL
GLOBAL CHAOS SYNCHRONIZATION OF PAN AND LÜ CHAOTIC SYSTEMS VIA ADAPTIVE CONTROL Sundarapandian Vaidyanathan 1 and Karthikeyan Rajagopal 2 1 Research and Development Centre, Vel Tech Dr. RR & Dr. SR Technical
More informationSynchronization of different chaotic systems and electronic circuit analysis
Synchronization of different chaotic systems and electronic circuit analysis J.. Park, T.. Lee,.. Ji,.. Jung, S.M. Lee epartment of lectrical ngineering, eungnam University, Kyongsan, Republic of Korea.
More informationChaos synchronization of nonlinear Bloch equations
Chaos, Solitons and Fractal7 (26) 357 361 www.elsevier.com/locate/chaos Chaos synchronization of nonlinear Bloch equations Ju H. Park * Robust Control and Nonlinear Dynamics Laboratory, Department of Electrical
More informationHybrid Projective Dislocated Synchronization of Liu Chaotic System Based on Parameters Identification
www.ccenet.org/ma Modern Applied Science Vol. 6, No. ; February Hybrid Projective Dilocated Synchronization of Liu Chaotic Sytem Baed on Parameter Identification Yanfei Chen College of Science, Guilin
More informationGlobal Chaos Synchronization of Hyperchaotic Lorenz and Hyperchaotic Chen Systems by Adaptive Control
Global Chaos Synchronization of Hyperchaotic Lorenz and Hyperchaotic Chen Systems by Adaptive Control Dr. V. Sundarapandian Professor, Research and Development Centre Vel Tech Dr. RR & Dr. SR Technical
More informationA New Finance Chaotic Attractor
ISSN 1749-3889(print),1749-3897(online) International Journal of Nonlinear Science Vol. 3 (2007) No. 3, pp. 213-220 A New Finance Chaotic Attractor Guoliang Cai +1,Juanjuan Huang 1,2 1 Nonlinear Scientific
More informationHopf bifurcations analysis of a three-dimensional nonlinear system
BULETINUL ACADEMIEI DE ŞTIINŢE A REPUBLICII MOLDOVA. MATEMATICA Number 358), 28, Pages 57 66 ISSN 124 7696 Hopf bifurcations analysis of a three-dimensional nonlinear system Mircea Craioveanu, Gheorghe
More informationCHALMERS, GÖTEBORGS UNIVERSITET. EXAM for DYNAMICAL SYSTEMS. COURSE CODES: TIF 155, FIM770GU, PhD
CHALMERS, GÖTEBORGS UNIVERSITET EXAM for DYNAMICAL SYSTEMS COURSE CODES: TIF 155, FIM770GU, PhD Time: Place: Teachers: Allowed material: Not allowed: August 22, 2018, at 08 30 12 30 Johanneberg Jan Meibohm,
More information