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Dec 2012

Volume 22, Issue 4, Articles (04xxxx)

Issue Cover Spotlight Figure

Chaos 22, 047510 (2012); http://dx.doi.org/10.1063/1.4772195 (33 pages)

Marko Budišić, Ryan Mohr, and Igor Mezić
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Introduction to the focus issue: Fifty years of chaos: Applied and theoretical

Takashi Hikihara, Philip Holmes, Tsutomu Kambe, and Giuseppe Rega

Chaos 22, 047501 (2012); http://dx.doi.org/10.1063/1.4769035 (4 pages)

Online Publication Date: 14 December 2012

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The discovery of deterministic chaos in the late nineteenth century, its subsequent study, and the development of mathematical and computational methods for its analysis have substantially influenced the sciences. Chaos is, however, only one phenomenon in the larger area of dynamical systems theory. This Focus Issue collects 13 papers, from authors and research groups representing the mathematical, physical, and biological sciences, that were presented at a symposium held at Kyoto University from November 28 to December 2, 2011. The symposium, sponsored by the International Union of Theoretical and Applied Mechanics, was called 50 Years of Chaos: Applied and Theoretical. Following some historical remarks to provide a background for the last 50 years, and for chaos, this Introduction surveys the papers and identifies some common themes that appear in them and in the theory of dynamical systems.
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01.30.-y Physics literature and publications
05.45.-a Nonlinear dynamics and chaos

Controlling practical stability and safety of mechanical systems by exploiting chaos properties

Stefano Lenci, Diego Orlando, Giuseppe Rega, and Paulo B. Gonçalves

Chaos 22, 047502 (2012); http://dx.doi.org/10.1063/1.4746094 (15 pages) | Cited 1 time

Online Publication Date: 14 December 2012

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In this paper, a method for controlling the global nonlinear dynamics of mechanical systems is applied to two models: the model of Augusti and an inverted guyed pendulum. These simplified models represent a large class of structures liable to buckling exhibiting interacting buckling phenomena. These structures may fail at load levels well below the theoretical buckling load due to complex nonlinear phenomena that decrease the safety and the dynamic integrity of the structure; this often occur as a consequence of imperfections and of the erosion of the basins of attraction of the safe pre-buckling solutions. So, it is of paramount practical importance to increase the safety of these structures in a dynamic environment. This can be achieved by increasing the integrity of the basins of attraction of the safe solutions, a goal that is attained by a control method which consists of the (optimal) elimination of homoclinic (or heteroclinic) intersection by properly adding superharmonic terms to a given harmonic excitation. By means of the solution of an appropriate optimization problem, it is possible to select the amplitudes and the phases of the added superharmonics in such a way that the manifolds distance is as large as possible. The results show that this methodology increases the integrity of the basins of attraction of the system and, consequently, the practical safety of the structure.
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05.45.Gg Control of chaos, applications of chaos
46.32.+x Static buckling and instability
02.30.Oz Bifurcation theory
05.45.Df Fractals

Synchronous rotation of the set of double pendula: Experimental observations

J. Strzalko, J. Grabski, J. Wojewoda, M. Wiercigroch, and T. Kapitaniak

Chaos 22, 047503 (2012); http://dx.doi.org/10.1063/1.4740460 (7 pages) | Cited 1 time

Online Publication Date: 14 December 2012

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We study the occurrence of the synchronous rotation of a set of four uncoupled nonidentical double pendula arranged into a cross structure mounted on a vertically excited platform. Under the excitation, the pendula can rotate in different directions (counter-clockwise or clockwise). It has been shown that after a transient, many different types of synchronous configurations with the constant phase difference between pendula can be observed. The experimental results qualitatively agree with the numerical simulations.
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05.45.Xt Synchronization; coupled oscillators

The three-dimensional dynamics of the die throw

M. Kapitaniak, J. Strzalko, J. Grabski, and T. Kapitaniak

Chaos 22, 047504 (2012); http://dx.doi.org/10.1063/1.4746038 (8 pages) | Cited 2 times

Online Publication Date: 14 December 2012

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A three-dimensional model of a die throw which considers the die bounces with dissipation on the fixed and oscillating table has been formulated. It allows simulations of the trajectories for dice with different shapes. Numerical results have been compared with the experimental observation using high speed camera. It is shown that for the realistic values of the initial energy the probabilities of the die landing on the face which is the lowest one at the beginning is larger than the probabilities of landing on any other face. We argue that non-smoothness of the system plays a key role in the occurrence of dynamical uncertainties and gives the explanation why for practically small uncertainties in the initial conditions a mechanical randomizer approximates the random process.
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05.40.-a Fluctuation phenomena, random processes, noise, and Brownian motion
02.50.-r Probability theory, stochastic processes, and statistics

Periodic orbits near onset of chaos in plane Couette flow

Tobias Kreilos and Bruno Eckhardt

Chaos 22, 047505 (2012); http://dx.doi.org/10.1063/1.4757227 (8 pages) | Cited 5 times

Online Publication Date: 14 December 2012

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We track the secondary bifurcations of coherent states in plane Couette flow and show that they undergo a periodic doubling cascade that ends with a crisis bifurcation. We introduce a symbolic dynamics for the orbits and show that the ones that exist fall into the universal sequence described by Metropolis, Stein and Stein for unimodal maps. The periodic orbits cover much of the turbulent dynamics in that their temporal evolution overlaps with turbulent motions when projected onto a plane spanned by energy production and dissipation.
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05.45.-a Nonlinear dynamics and chaos

Cartography of high-dimensional flows: A visual guide to sections and slices

Predrag Cvitanović, Daniel Borrero-Echeverry, Keith M. Carroll, Bryce Robbins, and Evangelos Siminos

Chaos 22, 047506 (2012); http://dx.doi.org/10.1063/1.4758309 (10 pages) | Cited 2 times

Online Publication Date: 14 December 2012

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Symmetry reduction by the method of slices quotients the continuous symmetries of chaotic flows by replacing the original state space by a set of charts, each covering a neighborhood of a dynamically important class of solutions, qualitatively captured by a “template.” Together these charts provide an atlas of the symmetry-reduced “slice” of state space, charting the regions of the manifold explored by the trajectories of interest. Within the slice, relative equilibria reduce to equilibria and relative periodic orbits reduce to periodic orbits. Visualizations of these solutions and their unstable manifolds reveal their interrelations and the role they play in organizing turbulence/chaos.
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47.52.+j Chaos in fluid dynamics
05.45.Jn High-dimensional chaos
47.10.ad Navier-Stokes equations

Dynamics of partial control

Juan Sabuco, Miguel A. F. Sanjuán, and James A. Yorke

Chaos 22, 047507 (2012); http://dx.doi.org/10.1063/1.4754874 (9 pages) | Cited 1 time

Online Publication Date: 14 December 2012

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Safe sets are a basic ingredient in the strategy of partial control of chaotic systems. Recently we have found an algorithm, the sculpting algorithm, which allows us to construct them, when they exist. Here we define another type of set, an asymptotic safe set, to which trajectories are attracted asymptotically when the partial control strategy is applied. We apply all these ideas to a specific example of a Duffing oscillator showing the geometry of these sets in phase space. The software for creating all the figures appearing in this paper is available as supplementary material.
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05.45.-a Nonlinear dynamics and chaos

Combinatorial-topological framework for the analysis of global dynamics

Justin Bush, Marcio Gameiro, Shaun Harker, Hiroshi Kokubu, Konstantin Mischaikow, Ippei Obayashi, and Paweł Pilarczyk

Chaos 22, 047508 (2012); http://dx.doi.org/10.1063/1.4767672 (16 pages) | Cited 1 time

Online Publication Date: 14 December 2012

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We discuss an algorithmic framework based on efficient graph algorithms and algebraic-topological computational tools. The framework is aimed at automatic computation of a database of global dynamics of a given m-parameter semidynamical system with discrete time on a bounded subset of the n-dimensional phase space. We introduce the mathematical background, which is based upon Conley's topological approach to dynamics, describe the algorithms for the analysis of the dynamics using rectangular grids both in phase space and parameter space, and show two sample applications.
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02.40.Re Algebraic topology
02.10.Ox Combinatorics; graph theory

Particle filtering in high-dimensional chaotic systems

Nishanth Lingala, N. Sri Namachchivaya, Nicolas Perkowski, and Hoong C. Yeong

Chaos 22, 047509 (2012); http://dx.doi.org/10.1063/1.4766595 (18 pages) | Cited 1 time

Online Publication Date: 14 December 2012

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We present an efficient particle filtering algorithm for multiscale systems, which is adapted for simple atmospheric dynamics models that are inherently chaotic. Particle filters represent the posterior conditional distribution of the state variables by a collection of particles, which evolves and adapts recursively as new information becomes available. The difference between the estimated state and the true state of the system constitutes the error in specifying or forecasting the state, which is amplified in chaotic systems that have a number of positive Lyapunov exponents. In this paper, we propose a reduced-order particle filtering algorithm based on the homogenized multiscale filtering framework developed in Imkeller et al. “Dimensional reduction in nonlinear filtering: A homogenization approach,” Ann. Appl. Probab. (to be published). In order to adapt the proposed algorithm to chaotic signals, importance sampling and control theoretic methods are employed for the construction of the proposal density for the particle filter. Finally, we apply the general homogenized particle filtering algorithm developed here to the Lorenz'96 [E. N. Lorenz, “Predictability: A problem partly solved,” in Predictability of Weather and Climate, ECMWF, 2006 (ECMWF, 2006), pp. 40–58] atmospheric model that mimics mid-latitude atmospheric dynamics with microscopic convective processes.
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05.45.-a Nonlinear dynamics and chaos
02.50.-r Probability theory, stochastic processes, and statistics
02.60.-x Numerical approximation and analysis
FREE

Applied Koopmanism

Marko Budišić, Ryan Mohr, and Igor Mezić

Chaos 22, 047510 (2012); http://dx.doi.org/10.1063/1.4772195 (33 pages) | Cited 1 time

Online Publication Date: 21 December 2012

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A majority of methods from dynamical system analysis, especially those in applied settings, rely on Poincaré's geometric picture that focuses on “dynamics of states.” While this picture has fueled our field for a century, it has shown difficulties in handling high-dimensional, ill-described, and uncertain systems, which are more and more common in engineered systems design and analysis of “big data” measurements. This overview article presents an alternative framework for dynamical systems, based on the “dynamics of observables” picture. The central object is the Koopman operator: an infinite-dimensional, linear operator that is nonetheless capable of capturing the full nonlinear dynamics. The first goal of this paper is to make it clear how methods that appeared in different papers and contexts all relate to each other through spectral properties of the Koopman operator. The second goal is to present these methods in a concise manner in an effort to make the framework accessible to researchers who would like to apply them, but also, expand and improve them. Finally, we aim to provide a road map through the literature where each of the topics was described in detail. We describe three main concepts: Koopman mode analysis, Koopman eigenquotients, and continuous indicators of ergodicity. For each concept, we provide a summary of theoretical concepts required to define and study them, numerical methods that have been developed for their analysis, and, when possible, applications that made use of them. The Koopman framework is showing potential for crossing over from academic and theoretical use to industrial practice. Therefore, the paper highlights its strengths in applied and numerical contexts. Additionally, we point out areas where an additional research push is needed before the approach is adopted as an off-the-shelf framework for analysis and design.
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05.45.-a Nonlinear dynamics and chaos
02.40.-k Geometry, differential geometry, and topology
02.60.-x Numerical approximation and analysis

Chaos in neurons and its application: Perspective of chaos engineering

Yoshito Hirata, Makito Oku, and Kazuyuki Aihara

Chaos 22, 047511 (2012); http://dx.doi.org/10.1063/1.4738191 (7 pages) | Cited 1 time

Online Publication Date: 21 December 2012

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We review our recent work on chaos in neurons and its application to neural networks from perspective of chaos engineering. Especially, we analyze a dataset of a squid giant axon by newly combining our previous work of identifying Devaney’s chaos with surrogate data analysis, and show that an axon can behave chaotically. Based on this knowledge, we use a chaotic neuron model to investigate possible information processing in the brain.
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05.45.-a Nonlinear dynamics and chaos
FREE

β-expansion attractors observed in A/D converters

Tohru Kohda, Yoshihiko Horio, and Kazuyuki Aihara

Chaos 22, 047512 (2012); http://dx.doi.org/10.1063/1.4758813 (18 pages) | Cited 1 time

Online Publication Date: 21 December 2012

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The recently proposed β-encoders, analog-to-digital converters using an amplifier with a factor β and a flaky quantizer with threshold ν, have proven to be explained by the deterministic dynamics of multi-valued Rényi-Parry maps. Such a map is locally eventually onto [ν−1, ν), which is topologically conjugate to Parry's (β,α)-map with α = (β−1)(ν−1). This implies that β-encoders have a closed subinterval [ν−1,ν), which includes an attractor. Thus, the iteration of the multi-valued Rényi-Parry map performs the β-expansion of x while quantization errors in β-encoders behave chaotically and do not converge to a fixed point. This β-expansion attractor is relatively simpler than previously reported attractors. The object of this paper is twofold: to observe the embedded attractors in the β-encoder and to identify attractors that are useful for spread-spectrum codes and optimization techniques using pseudo-random numbers.
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84.30.-r Electronic circuits
02.60.Pn Numerical optimization
FREE

Noise amplification by chaotic dynamics in a delayed feedback laser system and its application to nondeterministic random bit generation

Satoshi Sunada, Takahisa Harayama, Peter Davis, Ken Tsuzuki, Ken-ichi Arai, Kazuyuki Yoshimura, and Atsushi Uchida

Chaos 22, 047513 (2012); http://dx.doi.org/10.1063/1.4754872 (9 pages) | Cited 1 time

Online Publication Date: 21 December 2012

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We present an experimental method for directly observing the amplification of microscopic intrinsic noise in a high-dimensional chaotic laser system, a laser with delayed feedback. In the experiment, the chaotic laser system is repeatedly switched from a stable lasing state to a chaotic state, and the time evolution of an ensemble of chaotic states starting from the same initial state is measured. It is experimentally demonstrated that intrinsic noises amplified by the chaotic dynamics are transformed into macroscopic fluctuating signals, and the probability density of the output light intensity actually converges to a natural invariant probability density in a strongly chaotic regime. Moreover, with the experimental method, we discuss the application of the chaotic laser systems to physical random bit generators. It is experimentally shown that the convergence to the invariant density plays an important role in nondeterministic random bit generation, which could be desirable for future ultimate secure communication systems.
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42.65.Sf Dynamics of nonlinear optical systems; optical instabilities, optical chaos and complexity, and optical spatio-temporal dynamics
42.55.Px Semiconductor lasers; laser diodes
42.60.By Design of specific laser systems
42.60.Da Resonators, cavities, amplifiers, arrays, and rings

Nonlinear channelizer

Visarath In, Patrick Longhini, Andy Kho, Joseph D. Neff, Daniel Leung, Norman Liu, Brian K. Meadows, Frank Gordon, Adi R. Bulsara, and Antonio Palacios

Chaos 22, 047514 (2012); http://dx.doi.org/10.1063/1.4750032 (12 pages) | Cited 1 time

Online Publication Date: 21 December 2012

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The nonlinear channelizer is an integrated circuit made up of large parallel arrays of analog nonlinear oscillators, which, collectively, serve as a broad-spectrum analyzer with the ability to receive complex signals containing multiple frequencies and instantaneously lock-on or respond to a received signal in a few oscillation cycles. The concept is based on the generation of internal oscillations in coupled nonlinear systems that do not normally oscillate in the absence of coupling. In particular, the system consists of unidirectionally coupled bistable nonlinear elements, where the frequency and other dynamical characteristics of the emergent oscillations depend on the system's internal parameters and the received signal. These properties and characteristics are being employed to develop a system capable of locking onto any arbitrary input radio frequency signal. The system is efficient by eliminating the need for high-speed, high-accuracy analog-to-digital converters, and compact by making use of nonlinear coupled systems to act as a channelizer (frequency binning and channeling), a low noise amplifier, and a frequency down-converter in a single step which, in turn, will reduce the size, weight, power, and cost of the entire communication system. This paper covers the theory, numerical simulations, and some engineering details that validate the concept at the frequency band of 1–4 GHz.
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84.30.Ng Oscillators, pulse generators, and function generators
84.30.Le Amplifiers
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