Concepedia

Publication | Open Access

Using machine learning to replicate chaotic attractors and calculate Lyapunov exponents from data

591

Citations

24

References

2017

Year

TLDR

The study proposes a reservoir‑computing based, model‑free method to estimate Lyapunov exponents of chaotic systems from data. The method feeds a short time series into a high‑dimensional reservoir, learns output weights via linear regression, then constructs an autonomous reservoir that reproduces the attractor’s climate, enabling analytic computation of its Lyapunov exponents. Tests on the Lorenz system show climate reproduction requires tuning reservoir parameters, while on the Kuramoto‑Sivashinsky equation the method successfully estimates the growing number of Lyapunov exponents as system size increases.

Abstract

We use recent advances in the machine learning area known as 'reservoir computing' to formulate a method for model-free estimation from data of the Lyapunov exponents of a chaotic process. The technique uses a limited time series of measurements as input to a high-dimensional dynamical system called a 'reservoir'. After the reservoir's response to the data is recorded, linear regression is used to learn a large set of parameters, called the 'output weights'. The learned output weights are then used to form a modified autonomous reservoir designed to be capable of producing arbitrarily long time series whose ergodic properties approximate those of the input signal. When successful, we say that the autonomous reservoir reproduces the attractor's 'climate'. Since the reservoir equations and output weights are known, we can compute derivatives needed to determine the Lyapunov exponents of the autonomous reservoir, which we then use as estimates of the Lyapunov exponents for the original input generating system. We illustrate the effectiveness of our technique with two examples, the Lorenz system, and the Kuramoto-Sivashinsky (KS) equation. In particular, we use the Lorenz system to show that achieving climate reproduction may require tuning of the reservoir parameters. For the case of the KS equation, we note that as the system's spatial size is increased, the number of Lyapunov exponents increases, thus yielding a challenging test of our method, which we find the method successfully passes.

References

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