Chaotic dynamics of three-dimensional DC magnetron discharge

1999 ◽  
Vol 27 (1) ◽  
pp. 92-93 ◽  
Author(s):  
S. Kondo ◽  
K. Nanbu
2014 ◽  
Vol 13 (2) ◽  
pp. 901-943 ◽  
Author(s):  
Ivan C. Christov ◽  
Richard M. Lueptow ◽  
Julio M. Ottino ◽  
Rob Sturman

Vacuum ◽  
1996 ◽  
Vol 47 (6-8) ◽  
pp. 1013-1016 ◽  
Author(s):  
K Nanbu ◽  
S Segawa ◽  
S Kondo

Author(s):  
Akroune Nourredine ◽  
◽  
Gharout Hacene ◽  
Prunaret Daniele-Fournier ◽  
Taha Abelkadous ◽  
...  

2020 ◽  
Vol 15 (11) ◽  
Author(s):  
Nataliya V. Stankevich ◽  
Natalya A. Shchegoleva ◽  
Igor R. Sataev ◽  
Alexander P. Kuznetsov

Abstract Using an example a system of two coupled generators of quasi-periodic oscillations, we study the occurrence of chaotic dynamics with one positive, two zero, and several negative Lyapunov exponents. It is shown that such dynamic arises as a result of a sequence of bifurcations of two-frequency torus doubling and involves saddle tori occurring at their doublings. This transition is associated with typical structure of parameter plane, like cross-road area and shrimp-shaped structures, based on the two-frequency quasi-periodic dynamics. Using double Poincaré section, we have shown destruction of three-frequency torus.


2016 ◽  
Vol 26 (12) ◽  
pp. 1650206 ◽  
Author(s):  
Haibo Jiang ◽  
Yang Liu ◽  
Zhouchao Wei ◽  
Liping Zhang

This paper studies a new class of three-dimensional maps in a Jerk-like structure with a special concern of their hidden chaotic dynamics. Our investigation focuses on the hidden chaotic attractors in three typical scenarios of fixed points, namely no fixed point, single fixed point, and two fixed points. A systematic computer search is performed to explore possible hidden chaotic attractors, and a number of examples of the proposed maps are used for demonstration. Numerical results show that the routes to hidden chaotic attractors are complex, and the basins of attraction for the hidden chaotic attractors could be tiny, so that using the standard computational procedure for localization is impossible.


2005 ◽  
Vol 15 (11) ◽  
pp. 3493-3508 ◽  
Author(s):  
S. V. GONCHENKO ◽  
I. I. OVSYANNIKOV ◽  
C. SIMÓ ◽  
D. TURAEV

We discuss a rather new phenomenon in chaotic dynamics connected with the fact that some three-dimensional diffeomorphisms can possess wild Lorenz-type strange attractors. These attractors persist for open domains in the parameter space. In particular, we report on the existence of such domains for a three-dimensional Hénon map (a simple quadratic map with a constant Jacobian which occurs in a natural way in unfoldings of several types of homoclinic bifurcations). Among other observations, we have evidence that there are different types of Lorenz-like attractor domains in the parameter space of the 3D Hénon map. In all cases the maximal Lyapunov exponent, Λ1, is positive. Concerning the next Lyapunov exponent, Λ2, there are open domains where it is definitely positive, others where it is definitely negative and, finally, domains where it cannot be distinguished numerically from zero (i.e. |Λ2| < ρ, where ρ is some tolerance ranging between 10-5 and 10-6). Furthermore, several other types of interesting attractors have been found in this family of 3D Hénon maps.


2000 ◽  
Vol 4 (4) ◽  
pp. 319-331 ◽  
Author(s):  
Toichiro Asada ◽  
Toichio Inaba ◽  
Tetsuya Misawa

In this paper, we formulate a discrete time version of the Kaldorian macrodynamic model in a small open economy with fixed exchange rates. The model is described by a system of the three-dimensional nonlinear difference equations with and without stochastic disturbances (noise effects). We study the local stability/instability properties analytically by using the linear approximation method, and chaotic dynamics with and without noise effects are investigated by means of numerical simulations. In general, it is believed that the effect of the noise is to obscure the basic structure of the system. But, this is not necessarily the case. We show by means of numerical analysis that the noise can reveal the hidden structure of the model contrary to the usual intuition in some situations.


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