Unfolding Preprocessing for Meaningful Time Series Clustering

Total Page:16

File Type:pdf, Size:1020Kb

Unfolding Preprocessing for Meaningful Time Series Clustering Neural Networks 19 (2006) 877–888 www.elsevier.com/locate/neunet 2006 Special Issue Unfolding preprocessing for meaningful time series clustering Geoffroy Simona,∗,1, John A. Leea,2, Michel Verleysena,b,3 a Machine Learning Group - DICE, Universite´ Catholique de Louvain, Place du Levant 3, B-1348 Louvain-la-Neuve, Belgium b SAMOS-MATISSE, UMR CNRS 8595, Universite´ Paris I - Pantheon´ Sorbonne, Rue de Tolbiac 90, F-75634 Paris Cedex 13, France Abstract Clustering methods are commonly applied to time series, either as a preprocessing stage for other methods or in their own right. In this paper it is explained why time series clustering may sometimes be considered as meaningless. This problematic situation is illustrated for various raw time series. The unfolding preprocessing methodology is then introduced. The usefulness of unfolding preprocessing is illustrated for various time series. The experimental results show the meaningfulness of the clustering when applied on adequately unfolded time series. c 2006 Elsevier Ltd. All rights reserved. Keywords: Clustering; Time series; Self-organizing maps 1. Introduction be extracted from the series using a sliding window. In the remainder of the text vectors of successive past values are called Time series analysis is a task encountered in many fields, regressors. for example mathematics, statistics, econometrics, system Despite the frequent use of these clustering methods on time identification, physics and machine learning to cite only a few. series very few works try to answer fundamental questions such In all these fields there exist various methods of analyzing, as the meaningfulness of time series clustering. Recently it has describing, extracting features or even forecasting time series. been proved that in some cases clustering on time series is Among all these data analysis tools the partitioning, vector meaningless (Keogh, Lin, & Truppel, 2003). Some authors used quantization and similarity search methods can be grouped this proof to conclude that subsequence or regressor clustering under the general heading of clustering methods. is always meaningless (Bagnall, Janakec, & Zhang, 2003; Clustering is usually applied to time series in two different Hetland, 2003; Mahoney & Chan, 2005). It is shown in Struzik ways. In the context of time series prediction, for example, (2003) that time series clustering is not meaningless but rather clustering can be applied to time series either as preprocessing difficult due to the auto-similarity of the series. It is also proved for another time series prediction model (Cottrell, Girard, & in Denton (2004) that kernel-based clustering methods are able Rousset, 1997; Vesanto, 1997) or (Dablemont et al., 2003) for to provide meaningful clustering for time series. In this paper example) or as a prediction model in its own right ((Martinetz, it will be shown that clustering is indeed meaningful once the Berkovich, & Schulten, 1993; Simon, Lendasse, Cottrell, Fort, regressors are unfolded, i.e. when some adequate preprocessing & Verleysen, 2004; Walter, Ritter, & Schulten, 1990) to cite is performed. only a few references). In practice most of the clustering In order to show the meaningfulness of clustering the methods work with subsequences of the initial time series. Such unfolding preprocessing is introduced. This methodology is subsequences are vectors of successive past values that can based on embedding (Sauer, Yorke, & Casdagli, 1991). The main idea of embedding is to use delayed coordinates in the ∗ regressors. Selection of the optimal delay can be done using Corresponding author. either the autocorrelation function (Abarbanel, 1997; Kantz & E-mail address: [email protected] (G. Simon). URL: http://www.dice.ucl.ac.be/∼gsimon/ (G. Simon). Schreiber, 1997; Kaplan & Glass, 1995) or mutual information 1 G. Simon is funded by the Belgian F.R.I.A. (Abarbanel, 1997; Fraser & Swinney, 1986; Kantz & Schreiber, 2 J.A. Lee is a Scientific Research Worker of the Belgian F.N.R.S. 1997). The limit of these two common approaches is that the 3 M. Verleysen is a Research Director of the Belgian F.N.R.S. first lag is usually selected with great care but the influence 0893-6080/$ - see front matter c 2006 Elsevier Ltd. All rights reserved. doi:10.1016/j.neunet.2006.05.020 878 G. Simon et al. / Neural Networks 19 (2006) 877–888 of the other delayed components (selected using multiples of cross-validation, bootstrap (Efron & Tibshirani, 1993)) are also this lag) is not taken into account. In this paper a measure is often used in order to find a correct value for the model proposed to determine whether the selected delay is sufficient complexity p. Another approach to choose p is to estimate the to unfold efficiently the series in a p-dimensional space of dimension of the time series using the correlation dimension, regressors. The idea of the proposed criterion is to observe the as proposed in Ding, Grebogi, Ott, Sauer, and Yorke (1993), mean distance of a data set to the principal diagonal of its space. Grassberger and Procaccia (1983) and Sauer et al. (1991) The whole methodology allows creating unfolded regressors and illustrated in Babloyantz, Nicolis, and Salazar (1985) with much more informative content than those obtained using and Camastra and Colla (1999) to cite only a few. However, the simple sliding window technique. The meaningfulness of this question of choosing an adequate value of p is quite time series clustering on these unfolded time series will then be independent from the unfolding goal of this work; p will shown on artificial and real time series using a Self-Organizing therefore be deemed to be fixed a priori throughout the rest of Map (Kohonen, 1995). Self-Organizing Maps are used here as a this paper. clustering tool thanks to their vector quantization property. The meaningfulness of time series clustering will be observed using 2.2. Self-Organizing Maps criteria that measure the relative differences between regressor distributions. The Self-Organizing Map (SOM) algorithm is an unsuper- The paper is organized as follows. Notations and definitions vised classification algorithm proposed in the 1980s (Kohonen, are given in Section 2, which ends with a brief description 1995). Since its introduction it has been applied in many ar- of Self-Organizing Maps. The criterion to measure the eas, from classification to robotics to cite only two (Kohonen, meaningfulness of clustering is detailed in Section 3. The so- 1995). The intuitive graphical representations that can be ob- called ’meaninglessness’ of time series clustering is shown in tained from the SOM have made this tool a very popular non- the same section using graphical representations in 2- and 3- linear clustering method. Theoretical aspects of the SOM have dimensional spaces. The unfolding preprocessing methodology also been studied in detail (Cottrell, Fort, & Pages,` 1998). is presented and illustrated in Section 4. Experimental results The main concepts of the SOM algorithm can be are provided in Section 5. Section 6 concludes the paper. summarized as follows. During the learning stage, the SOM units, or prototypes, are moved within the data distribution. 2. Regressor clustering using Self-Organizing Maps Each prototype is linked to neighbouring ones according to a 1- or 2-dimensional grid whose shape and size are chosen 2.1. Time series and regressors: Definitions and notations a priori. The learning consists in presenting each datum and selecting the closest prototype with respect to some A time series S is a series of values xt , with 1 ≤ t ≤ distance measure. This winning prototype is moved towards n, measured from a time varying process. The xt values are ordered according to the time index and sampled with constant the data while its neighbours are also moved according to constraints given by the grid. At the end of the learning frequency. Note that, for reasons of simplicity, xt is considered as scalar here though it could be a multidimensional vector. stage, the final prototype positions represent a discrete and In the context of time series prediction one has to build a rough approximation of the data density that is therefore model of the series. For example regression models have at least partitioned into clusters. Each cluster is associated with one of one output and some inputs corresponding either to past values the prototypes. The two main properties of the SOM are vector quantization xt of the time series itself or to past values ut of other related processes. These inputs are grouped in a vector describing the and topology preservation. In this paper, the SOM is used as state of the process at a given time t and defined as: a clustering tool. Data to be clustered are the p-dimensional regressors obtained from the time series. t xt−p+1 = {xt , xt−1,..., xt−p+1, ut , ut−1,..., ut−q+1}. (1) 3. Why time series clustering may be considered as + t The p q-dimensional vector xt−p+1 is called the regressor. meaningless For reasons of simplicity the regressors will be limited in this paper to p-dimensional vectors of past values: How can the meaningfulness of time series clustering t be observed? Consider two different time series. Once the x = {x , x − ,..., x − + }. (2) t−p+1 t t 1 t p 1 regressors are formed for each series one can reasonably expect Intuitively, the regressors can be seen as subsequences obtained that the two sets of regressors are different as they describe two from the initial time series using a sliding window. distinct processes. Applying a clustering method like the SOM The question regarding how to choose the length p algorithm on both sets of regressors reduces the information of the regressor is decisive for the model. This question encoded in the regressors such that it is now contained can be answered elegantly for linear models using various in a limited number of prototypes.
Recommended publications
  • Research on the Digitial Image Based on Hyper-Chaotic And
    Research on digital image watermark encryption based on hyperchaos Item Type Thesis or dissertation Authors Wu, Pianhui Publisher University of Derby Download date 27/09/2021 09:45:19 Link to Item http://hdl.handle.net/10545/305004 UNIVERSITY OF DERBY RESEARCH ON DIGITAL IMAGE WATERMARK ENCRYPTION BASED ON HYPERCHAOS Pianhui Wu Doctor of Philosophy 2013 RESEARCH ON DIGITAL IMAGE WATERMARK ENCRYPTION BASED ON HYPERCHAOS A thesis submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy By Pianhui Wu BSc. MSc. Faculty of Business, Computing and Law University of Derby May 2013 To my parents Acknowledgements I would like to thank sincerely Professor Zhengxu Zhao for his guidance, understanding, patience and most importantly, his friendship during my graduate studies at the University of Derby. His mentorship was paramount in providing a well-round experience consistent with my long-term career goals. I am grateful to many people in Faculty of Business, Computing and Law at the University of Derby for their support and help. I would also like to thank my parents, who have given me huge support and encouragement. Their advice is invaluable. An extra special recognition to my sister whose love and aid have made this thesis possible, and my time in Derby a colorful and wonderful experience. I Glossary AC Alternating Current AES Advanced Encryption Standard CCS Combination Coordinate Space CWT Continue Wavelet Transform BMP Bit Map DC Direct Current DCT Discrete Cosine Transform DWT Discrete Wavelet Transform
    [Show full text]
  • Projective Synchronization of Chaotic Systems Via Backstepping Design
    International Journal of Applied Mathematical Research, 1 (4) (2012) 531-540 ©Science Publishing Corporation www.sciencepubco.com/index.php/IJBAS Projective Synchronization of Chaotic Systems Via Backstepping Design 1 Anindita Tarai (Poria), 2 Mohammad Ali Khan 1 Department of Mathematics, Aligunj R.R.B. High School Midnapore (West), West Bengal, India E-mail: [email protected] 2 Department of Mathematics, Garhbeta Ramsundar Vidyabhavan, Garhbeta, Midnapore (West), West Bengal, India E-mail: [email protected] Abstract Chaos synchronization of discrete dynamical systems are investigated. An algorithm is proposed for projective synchronization of chaotic 2D Duffing map and chaotic Tinkerbell map. The control law was derived from the Lyapunov stability theory. The numerical simulation results are presented to verify the effectiveness of the proposed algorithm Keywords: Lyapunov function, Projective synchronization, Backstepping Design, Duffing map and Tinkerbell map. 1 Introduction Adjacent chaotic trajectories governed by the same nonlinear systems may evolve into a state utterly uncorrelated, but in 1990 Pecora and Carrol [1] shown that it could be synchronized through a proper coupling. Since their seminal paper in 1990, chaos synchronization is an interesting research topic of great attention. Hayes et.al. (1993)[2] have studied to some potential applications in secure communication. Blasius et.al. [3] have observed complex dynamics and phase synchronization in spatially extended ecological systems in 1999 and system identification was investigated by Kocarev et.al. in 1996 [4]. Different forms of synchronization phenomena have been observed in a variety of chaotic systems, such as identical synchronization [1]. In 1996 Rosenblum et.al. [5] have studied phase synchronization of chaotic oscillators.
    [Show full text]
  • 65 Numerical Analysis
    e Q (e t o 5 M SectionsSet 1Q (Section 65)MR September 2012 65 NUMERICAL ANALYSIS MR2918625 65-06 FRecent advances in scientific computing and matrix analysis. Proceedings of the International Workshop held at the University of Macau, Macau, December 28{30, 2009. Edited by Xiao-Qing Jin, Hai-Wei Sun and Seak-Weng Vong. International Press, Somerville, MA; Higher Education Press, Beijing, 2011. xii+126 pp. ISBN 978-1-57146-202-2 Contents: Zheng-jian Bai and Xiao-qing Jin [Xiao Qing Jin1], A note on the Ulm-like method for inverse eigenvalue problems (1{7) MR2908437; Che-man Cheng [Che-Man Cheng], Kin-sio Fong [Kin-Sio Fong] and Io-kei Lok [Io-Kei Lok], Another proof for commutators with maximal Frobenius norm (9{14) MR2908438; Wai-ki Ching [Wai-Ki Ching] and Dong-mei Zhu [Dong Mei Zhu1], On high-dimensional Markov chain models for categorical data sequences with applications (15{34) MR2908439; Yan-nei Law [Yan Nei Law], Hwee-kuan Lee [Hwee Kuan Lee], Chao-qiang Liu [Chaoqiang Liu] and Andy M. Yip, An additive variational model for image segmentation (35{48) MR2908440; Hai-yong Liao [Haiyong Liao] and Michael K. Ng, Total variation image restoration with automatic selection of regularization parameters (49{59) MR2908441; Franklin T. Luk and San-zheng Qiao [San Zheng Qiao], Matrices and the LLL algorithm (61{69) MR2908442; Mila Nikolova, Michael K. Ng and Chi-pan Tam [Chi-Pan Tam], A fast nonconvex nonsmooth minimization method for image restoration and reconstruction (71{83) MR2908443; Gang Wu [Gang Wu1], Eigenvalues of certain augmented complex stochastic matrices with applications to PageRank (85{92) MR2908444; Yan Xuan and Fu-rong Lin, Clenshaw-Curtis-rational quadrature rule for Wiener-Hopf equations of the second kind (93{110) MR2908445; Man-chung Yeung [Man-Chung Yeung], On the solution of singular systems by Krylov subspace methods (111{116) MR2908446; Qi- fang Yu, San-zheng Qiao [San Zheng Qiao] and Yi-min Wei, A comparative study of the LLL algorithm (117{126) MR2908447.
    [Show full text]
  • Generalized Complexity Measures and Chaotic Maps B
    Generalized complexity measures and chaotic maps B. Godó and Á. Nagy Citation: Chaos 22, 023118 (2012); doi: 10.1063/1.4705088 View online: http://dx.doi.org/10.1063/1.4705088 View Table of Contents: http://chaos.aip.org/resource/1/CHAOEH/v22/i2 Published by the American Institute of Physics. Related Articles On finite-size Lyapunov exponents in multiscale systems Chaos 22, 023115 (2012) Exact folded-band chaotic oscillator Chaos 22, 023113 (2012) Components in time-varying graphs Chaos 22, 023101 (2012) Impulsive synchronization of coupled dynamical networks with nonidentical Duffing oscillators and coupling delays Chaos 22, 013140 (2012) Dynamics and transport in mean-field coupled, many degrees-of-freedom, area-preserving nontwist maps Chaos 22, 013137 (2012) Additional information on Chaos Journal Homepage: http://chaos.aip.org/ Journal Information: http://chaos.aip.org/about/about_the_journal Top downloads: http://chaos.aip.org/features/most_downloaded Information for Authors: http://chaos.aip.org/authors CHAOS 22, 023118 (2012) Generalized complexity measures and chaotic maps B. Godo´ and A´ . Nagy Department of Theoretical Physics, University of Debrecen, H–4010 Debrecen, Hungary (Received 24 November 2011; accepted 5 April 2012; published online 24 April 2012) The logistic and Tinkerbell maps are studied with the recently introduced generalized complexity measure. The generalized complexity detects periodic windows. Moreover, it recognizes the intersection of periodic branches of the bifurcation diagram. It also reflects the fractal character of the chaotic dynamics. There are cases where the complexity plot shows changes that cannot be seen in the bifurcation diagram. VC 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4705088] ð Complexity is a key concept in modern science.
    [Show full text]
  • A New Cost Function for Parameter Estimation of Chaotic Systems Using Return Maps As Fingerprints
    October 20, 2014 16:12 WSPC/S0218-1274 1450134 International Journal of Bifurcation and Chaos, Vol. 24, No. 10 (2014) 1450134 (18 pages) c World Scientific Publishing Company DOI: 10.1142/S021812741450134X A New Cost Function for Parameter Estimation of Chaotic Systems Using Return Maps as Fingerprints Sajad Jafari∗ Department of Biomedical Engineering, Amirkabir University of Technology, 424 Hafez Ave., Tehran 15875–4413, Iran [email protected] Julien C. Sprott Department of Physics, University of Wisconsin–Madison, Madison, WI 53706, USA [email protected] Viet-Thanh Pham School of Electronics and Telecommunications, Hanoi University of Science and Technology, 01 Dai Co Viet, Hanoi, Vietnam [email protected] S. Mohammad Reza Hashemi Golpayegani Department of Biomedical Engineering, Amirkabir University of Technology, 424 Hafez Ave., Tehran 15875–4413, Iran [email protected] Amir Homayoun Jafari by Prof. Clint Sprott on 11/07/14. For personal use only. Department of Medical Physics and Biomedical Engineering, Tehran University of Medical Sciences, Tehran 14155–6447, Iran Int. J. Bifurcation Chaos 2014.24. Downloaded from www.worldscientific.com h [email protected] Received May 30, 2014 Estimating parameters of a model system using observed chaotic scalar time series data is a topic of active interest. To estimate these parameters requires a suitable similarity indicator between the observed and model systems. Many works have considered a similarity measure in the time domain, which has limitations because of sensitive dependence on initial conditions. On the other hand, there are features of chaotic systems that are not sensitive to initial conditions such as the topology of the strange attractor.
    [Show full text]
  • Bogdanov Map for Modelling a Phase-Conjugated Ring Resonator
    entropy Article Bogdanov Map for Modelling a Phase-Conjugated Ring Resonator Vicente Aboites 1,* , David Liceaga 2, Rider Jaimes-Reátegui 3 and Juan Hugo García-López 3 1 Centro de Investigaciones en Óptica, Loma del Bosque 115, 37150 León, Mexico 2 División de Ciencias e Ingenierías, Universidad de Guanajuato, Loma del Bosque 107, 37150 León, Mexico; [email protected] 3 Centro Universitario de los Lagos, Universidad de Guadalajara, Enrique Diaz de León 1144, Paseos de la Montaña, Lagos de Moreno, 47460 Jalisco, Mexico; [email protected] (R.J.-R.); [email protected] (J.H.G.-L.) * Correspondence: [email protected]; Tel.: +52-4774414200 Received: 24 October 2018; Accepted: 4 December 2018; Published: 10 April 2019 Abstract: In this paper, we propose using paraxial matrix optics to describe a ring-phase conjugated resonator that includes an intracavity chaos-generating element; this allows the system to behave in phase space as a Bogdanov Map. Explicit expressions for the intracavity chaos-generating matrix elements were obtained. Furthermore, computer calculations for several parameter configurations were made; rich dynamic behavior among periodic orbits high periodicity and chaos were observed through bifurcation diagrams. These results confirm the direct dependence between the parameters present in the intracavity chaos-generating element. Keywords: spatial dynamics; Bogdanov Map; chaos; laser; resonator 1. Introduction Matrix description of optical systems through ABCD matrices (Equation (8)) naturally produces iterative maps with
    [Show full text]
  • Problems and Solutions in Nonlinear Dynamics, Chaos and Fractals
    Problems and Solutions in Nonlinear Dynamics, Chaos and Fractals by Willi-Hans Steeb International School for Scientific Computing at University of Johannesburg, South Africa Charles Villet Department of Applied Mathematics at University of Johannesburg, South Africa Yorick Hardy Department of Mathematical Sciences at University of South Africa, South Africa Ruedi Stoop Institute of Neuroinformatik University / ETH Z¨urich Contents 1 One-Dimensional Maps 1 1.1 Notations and Definitions . .1 1.2 One-Dimensional Maps . .6 1.2.1 Solved Problems . .6 1.2.2 Supplementary Problems . 37 2 Higher-Dimensional Maps and Complex Maps 48 2.1 Introduction . 48 2.2 Two-Dimensional Maps . 49 2.2.1 Solved Problems . 49 2.3 Complex Maps . 84 2.3.1 Solved Problems . 85 2.4 Higher Dimensional Maps . 91 2.4.1 Solved Problems . 91 2.5 Bitwise Problems . 94 2.6 Supplementary Problems . 97 3 Fractals 103 Bibliography 126 Index 139 vi Chapter 1 One-Dimensional Maps 1.1 Notations and Definitions We consider exercises for nonlinear one-dimensional maps. In particular we consider one-dimensional maps with chaotic behaviour. We first summa- rize the relevant definitions such as fixed points, stability, periodic orbit, Ljapunov exponent, invariant density, topologically conjugacy, etc.. Er- godic maps are also considered. We use the notation f : D ! C to indicate that a function f with domain D and codomain C. The notation f : D ! D indicates that the domain and codomain of the function are the same set. We also use the following two definitions: A mapping g : A 7! B is called surjective if g(A) = B.
    [Show full text]
  • Empirical Analysis of Robust Chaotic Maps for Image Encryption
    International Journal of Innovative Technology and Exploring Engineering (IJITEE) ISSN: 2278-3075, Volume-9 Issue-11, September 2020 Empirical Analysis of Robust Chaotic Maps for Image Encryption Sonal Ayyappan, C Lakshmi Abstract: The rate of transferring data in the form of text, image, video or audio over an open network has drastically increased. As these are carried out in highly sophisticated fields of medicine, military and banking, security becomes important. In- order to enhance security for transmission, encryption algorithms play a vital role. So as to enhance the proficiency of the existing Images are represented as 2-dimensional arrays of encryption methods and for stronger anti attack abilities, chaotic data. Hence to apply encryption algorithms it must be based cryptography is essential. Chaotic based encryption has considered as one-dimensional array of data[3]. One- advantages of being sensitive to initial conditions and control parameters. Images have features like bulk data capacity and high dimensional image array consumes more space when inter pixel correlation. Transmission of such medical data should compared to one dimensional text data which leads to be highly confidential, integral and authorized. Hence chaos-based compression. It results in reduced space and reduced time for image encryption is an efficient way of fast and high-quality image transmission. But this may cause loss of some data which encryption. It has features like good speed, complexity, highly may be agreeable for general images but may be costly for secure, reasonable computational overhead and power. In this medical images. This results to wrong diagnosis of these paper a comprehensive analysis and an evaluation regarding the medical images [4].
    [Show full text]
  • Attractors and Basins of Dynamical Systems
    Electronic Journal of Qualitative Theory of Differential Equations 2011, No. 20, 1-11; http://www.math.u-szeged.hu/ejqtde/ Attractors and basins of dynamical systems Attila D´enes, G´eza Makay Abstract There are several programs for studying dynamical systems, but none of them is very useful for investigating basins and attractors of higher dimensional systems. Our goal in this paper is to show a new algorithm for finding even chaotic attractors and their basins for these systems. We present an implementation and examples for the use of this program. Key words: dynamical systems, attractors, basins, numerical methods. 2000 Mathematics Subject Classification: Primary 37D45, 37M99. 1 Introduction There exist several program packages for investigating dynamical systems. However, we found that even the most widespread of these are not suitable for the examination of attractors and basins of dynamical systems. For ex- ample, Dynamica written in Mathematica [2] does not contain a procedure for representing attractors and basins. Dynamics [1] does have such a proce- dure, but as it was written under DOS, it is rather difficult to use on today’s computers, and the algorithm has some inadequacies that – in some cases – can cause imperfect results. For this reason we established a new algorithm and its computer realization to find and visualize attractors and basins of discrete and continuous dynamical systems. In Section 2 we introduce some basic notions from the theory of dynam- ical systems. As our algorithm is based on that of Dynamics, in Section 3 we describe the routine Basins and Attractors of Dynamics for representing attractors and their basins.
    [Show full text]
  • Microcontroller-Based Random Number Generator Implementation by Using Discrete Chaotic Maps
    Sakarya University Journal of Science ISSN 1301-4048 | e-ISSN 2147-835X | Period Bimonthly | Founded: 1997 | Publisher Sakarya University | http://www.saujs.sakarya.edu.tr/en/ Title: Microcontroller-based Random Number Generator Implementation by Using Discrete Chaotic Maps Authors: Serdar ÇİÇEK Recieved: 2020-04-27 03:59:56 Accepted: 2020-06-17 14:47:55 Article Type: Research Article Volume: 24 Issue: 5 Month: October Year: 2020 Pages: 832-844 How to cite Serdar ÇİÇEK; (2020), Microcontroller-based Random Number Generator Implementation by Using Discrete Chaotic Maps. Sakarya University Journal of Science, 24(5), 832-844, DOI: https://doi.org/10.16984/saufenbilder.727449 Access link http://www.saujs.sakarya.edu.tr/en/pub/issue/56422/727449 New submission to SAUJS http://dergipark.org.tr/en/journal/1115/submission/step/manuscript/new Sakarya University Journal of Science 24(5), 832-844, 2020 Microcontroller-based Random Number Generator Implementation by Using Discrete Chaotic Maps Serdar ÇİÇEK*1 Abstract In recent decades, chaos theory has been used in different engineering applications of different disciplines. Discrete chaotic maps can be used in encryption applications for digital applications. In this study, firstly, Lozi, Tinkerbell and Barnsley Fern discrete chaotic maps are implemented based on microcontroller. Then, microcontroller based random number generator is implemented by using the three different two-dimensional discrete chaotic maps. The designed random number generator outputs are applied to NIST (National Institute of Standards and Technology) 800-22 and FIPS (Federal Information Processing Standard) tests for randomness validity. The random numbers are successful in all tests. Keywords: Chaotic map, Random number generators, NIST 800-22, FIPS, Microcontroller 1.
    [Show full text]
  • Bifurcation, Chaos Analysis and Control in a Discrete-Time Predator–Prey System
    Liu and Cai Advances in Difference Equations (2019)2019:11 https://doi.org/10.1186/s13662-019-1950-6 R E S E A R C H Open Access Bifurcation, chaos analysis and control in a discrete-time predator–prey system Weiyi Liu1* and Donghan Cai1 *Correspondence: [email protected] Abstract 1School of Mathematics and Statistics, Wuhan University, Wuhan, The dynamical behavior of a discrete-time predator–prey model with modified China Leslie–Gower and Holling’s type II schemes is investigated on the basis of the normal form method as well as bifurcation and chaos theory. The existence and stability of fixed points for the model are discussed. It is showed that under certain conditions, the system undergoes a Neimark–Sacker bifurcation when bifurcation parameter passes a critical value, and a closed invariant curve arises from a fixed point. Chaos in the sense of Marotto is also verified by both analytical and numerical methods. Furthermore, to delay or eliminate the bifurcation and chaos phenomena that exist objectively in this system, two control strategies are designed, respectively. Numerical simulations are presented not only to validate analytical results but also to show the complicated dynamical behavior. MSC: Primary 37N25; secondary 34H10; 34H15; 34H20; 37M20; 39A28 Keywords: Predator–prey model; Local stability; Neimark–Sacker bifurcation; Marotto’s chaos; Bifurcation control; Chaos control 1 Introduction Predation is a common and very important species interaction in many biological systems. Mathematical models are useful tools to understand and analyze the dynamical behavior of the predator–prey system, among which the Lotka–Volterra model is the oldest and the best known representative.
    [Show full text]
  • Chaos and Time-Series Analysis OXTORD
    Chaos and Time-Series Analysis Julien Clinton Sprott Department of Physics Universitv of Wisconsin—Madison OXTORD UNIVERSITY PRESS Contents Introduction 1.1 Examples of dynamical systems 1.1.1 Astronomical systems 1.1.2 The Solar System 1.1.3 Fluids 1.1.4 Nonphysical systems 1.2 Driven pendulum 1.3 Ball on an oscillating floor 1.4 Dripping faucet 1.5 Chaotic electrical circuits 1.5.1 Inductor-diode circuit 1.5.2 Chua's circuit 1.5.3 Jerk circuits 1.5.4 Relaxation oscillators 1.6 Other demonstrations of chaos 1.7 Exercises 1.8 Computer project: The logistic equation One-dimensional maps 2.1 Exponential growth in discrete time 2.2 The logistic equation 2.3 Bifurcations in the logistic map 2.3.1 0 < .4 < 1 case 2.3.2 1 < .4 < 3 case 2.3.3 3 < A < 3.44948... case 2.3.4 3.44948 ...< A< 3.56994 ... case 2.3.5 3.56994... < A < 4 case 2.3.6 A = 4 case 2.3.7 A > 4 case 2.4 Other properties of the logistic map with .4 2.4.1 Unstable periodic orbits 2.4.2 Eventually fixed points 2.4.3 Eventually periodic: points 2.4.4 Probability distribution 2.4.5 Nonrecursive representation 2.5 Other one-dimensional maps 2.5.1 Sine map x Contents 2.5.2 Tent map 2.5.3 General symmetric map 2.5.4 Binary shift map 2.6 Computer random-number generators 2.7 Exercises 2.8 Computer project: Bifurcation diagrams 3 Nonchaotic multi-dimensional flows 3.1 Exponential growth in continuous time 3.2 Logistic differential equation 3.3 Circular motion 3.4 Simple harmonic oscillator 3.5 Driven harmonic oscillator 3.6 Damped harmonic oscillator 3.6.1 Overdamped case 3.6.2 Critically
    [Show full text]