Stabilizing the unstable periodic orbits of a chaotic system using adaptive time-delayed state feedback

Author(s):  
Aida Fourati ◽  
Moez Feki
2009 ◽  
Vol 14 (12) ◽  
pp. 4273-4279 ◽  
Author(s):  
Arūnas Tamaševičius ◽  
Elena Tamaševičiūtė ◽  
Tatjana Pyragienė ◽  
Gytis Mykolaitis ◽  
Skaidra Bumelienė

1999 ◽  
Vol 38 (1) ◽  
pp. 21-26 ◽  
Author(s):  
Yang Genke ◽  
Wei Shuzhi ◽  
Wei Junhu ◽  
Zeng Jianchao ◽  
Wu Zhiming ◽  
...  

2008 ◽  
Vol 18 (11) ◽  
pp. 3485-3494 ◽  
Author(s):  
GUOSI HU ◽  
SHIQIN JIANG

This letter presents a new hyperchaotic system, which was constructed by adding an approximate time delayed state feedback to the second equation of Lorenz chaotic system. The constructed system is not only demonstrated by numerical simulations but also implemented via an electronic circuit, showing very good agreement with the simulation results.


2001 ◽  
Vol 11 (01) ◽  
pp. 215-224 ◽  
Author(s):  
TETSUSHI UETA ◽  
GUANRONG CHEN ◽  
TOHRU KAWABE

This paper describes a simple method for calculating unstable periodic orbits (UPOs) and their control in piecewise-linear autonomous systems. The algorithm can be used to obtain any desired UPO embedded in a chaotic attractor, and the UPO can be stabilized by a simple state feedback control. A brief stability analysis of the controlled system is also given.


1995 ◽  
Vol 05 (01) ◽  
pp. 281-295 ◽  
Author(s):  
ZBIGNIEW GALIAS

In this paper we present a new method of controlling periodic orbits in chaotic systems. This method can be applied in situations when the chaotic system depends on one system parameter, which can be changed over a continuous interval or over a discrete, two-element set. We compare the new method to other ones, discuss its properties, and illustrate our approach with a numerical example.


2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Saúl Pilatowsky-Cameo ◽  
David Villaseñor ◽  
Miguel A. Bastarrachea-Magnani ◽  
Sergio Lerma-Hernández ◽  
Lea F. Santos ◽  
...  

AbstractIn a classically chaotic system that is ergodic, any trajectory will be arbitrarily close to any point of the available phase space after a long time, filling it uniformly. Using Born’s rules to connect quantum states with probabilities, one might then expect that all quantum states in the chaotic regime should be uniformly distributed in phase space. This simplified picture was shaken by the discovery of quantum scarring, where some eigenstates are concentrated along unstable periodic orbits. Despite that, it is widely accepted that most eigenstates of chaotic models are indeed ergodic. Our results show instead that all eigenstates of the chaotic Dicke model are actually scarred. They also show that even the most random states of this interacting atom-photon system never occupy more than half of the available phase space. Quantum ergodicity is achievable only as an ensemble property, after temporal averages are performed.


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