Standard map

The phase-space of the standard map with the variation of the parameter

K

from 0 to 5.19 (

p_{n}

in y axes,

\theta_n

in x axes). Notice the appearance of a "dotted" zone, a signature of chaotic behavior.

Orbits of the standard map for K = 0.6.

Orbits of the standard map for K = 0.971635.

Orbits of the standard map for K = 1.2.

Orbits of the standard map for K = 2.0. The large green region is the main chaotic region of the map.

A single orbit of the standard map for K=2.0. Magnified close-up centered at

\theta=0.282

, p = 0.666, of total width/height 0.02. Note the extremely uniform distribution of the orbit.

The standard map (also known as the Chirikov–Taylor map or as the Chirikov standard map) is an area-preserving chaotic map from a square with side $2\pi$ onto itself.^[1] It is constructed by a Poincaré's surface of section of the kicked rotator, and is defined by:

p_{n+1} = p_n + K \sin(\theta_n)

\theta_{n+1} = \theta_n + p_{n+1}

where $p_{n}$ and $\theta_n$ are taken modulo $2\pi$ .

The properties of chaos of the standard map were established by Boris Chirikov in 1969. See more details at Scholarpedia entry.

Physical model

This map describes the Poincaré's surface of section of the motion of a simple mechanical system known as the kicked rotator. The kicked rotator consists of a stick that is free of the gravitational force, which can rotate frictionlessly in a plane around an axis located in one of its tips, and which is periodically kicked on the other tip.

The standard map is a surface of section applied by a stroboscopic projection on the variables of the kicked rotator.^[1] The variables $\theta_n$ and $p_{n}$ respectively determine the angular position of the stick and its angular momentum after the n-th kick. The constant K measures the intensity of the kicks on the kicked rotator.

The kicked rotator approximates systems studied in the fields of mechanics of particles, accelerator physics, plasma physics, and solid state physics. For example, circular particle accelerators accelerate particles by applying periodic kicks, as they circulate in the beam tube. Thus, the structure of the beam can be approximated by the kicked rotor. However, this map is interesting from a fundamental point of view in physics and mathematics because it is a very simple model of a conservative system that displays Hamiltonian chaos. It is therefore useful to study the development of chaos in this kind of system.

Main properties

For $K=0$ the map is linear and only periodic and quasiperiodic orbits are possible. When plotted in phase space (the θ–p plane), periodic orbits appear as closed curves, and quasiperiodic orbits as necklaces of closed curves whose centers lie in another larger closed curve. Which type of orbit is observed depends on the map's initial conditions.

Nonlinearity of the map increases with K, and with it the possibility to observe chaotic dynamics for appropriate initial conditions. This is illustrated in the figure, which displays a collection of different orbits allowed to the standard map for various values of $K>0$ . All the orbits shown are periodic or quasiperiodic, with the exception of the green one that is chaotic and develops in a large region of phase space as an apparently random set of points. Particularly remarkable is the extreme uniformity of the distribution in the chaotic region, although this can be deceptive: even within the chaotic regions, there are an infinite number of diminishingly small islands that are never visited during iteration, as shown in the close-up.

Circle map

The standard map is related to the circle map, which has a single, similar iterated equation:

\theta_{n+1} = \theta_n + \Omega - K \sin(\theta_n)

as compared to

\theta_{n+1} = \theta_n + p_n + K \sin(\theta_n)

p_{n+1} = \theta_{n+1} - \theta_{n}

for the standard map, the equations reordered to emphasize similarity. In essence, the circle map forces the momentum to a constant.

Notes

1 2 Ott, Edward (2002). Chaos in Dynamical Systems. Cambridge University Press New, York. ISBN 0-521-01084-5.

References

Chirikov, B.V. Research concerning the theory of nonlinear resonance and stochasticity. Preprint N 267, Institute of Nuclear Physics, Novosibirsk (1969) (in Russian) [Engl. Transl., CERN Trans. 71 - 40, Geneva, October (1971), Translated by A.T.Sanders]. link
Chirikov, B.V. A universal instability of many-dimensional oscillator systems. Phys. Rep. v.52. p.263 (1979) Elsvier, Amsterdam.
Lichtenberg, A.J. & Lieberman, M.A. (1992). Regular and Chaotic Dynamics. Springer, Berlin. ISBN 978-0-387-97745-4. Springer link
Ott, Edward (2002). Chaos in Dynamical Systems. Cambridge University Press New, York. ISBN 0-521-01084-5.
Sprott, Julien Clinton (2003). Chaos and Time-Series Analysis. Oxford University Press. ISBN 0-19-850840-9.

External links

Standard map at MathWorld
Chirikov standard map at Scholarpedia
Website dedicated to Boris Chirikov
Interactive Java Applet visualizing orbits of the Standard Map, by Achim Luhn
Mac Application for the Standard Map, by James Meiss
Interactive Javavascript Applet Standard Map on experiences.math.cnrs.fr

Chaos theory

Chaos theory	Anosov diffeomorphism Bifurcation theory Butterfly effect Chaos theory in organizational development Complexity Control of chaos Dynamical system Edge of chaos Fractal Predictability Quantum chaos Santa Fe Institute Synchronization of chaos Unintended consequences

Chaotic maps (list)	Arnold tongue Arnold's cat map Baker's map Complex quadratic map Complex squaring map Coupled map lattice Double pendulum Double scroll attractor Duffing equation Duffing map Dyadic transformation Dynamical billiards outer Exponential map Gauss map Gingerbreadman map Hénon map Horseshoe map Ikeda map Interval exchange map Kaplan–Yorke map Logistic map Lorenz system Multiscroll attractor Rabinovich–Fabrikant equations Rössler attractor Standard map Swinging Atwood's machine Tent map Tinkerbell map Van der Pol oscillator Zaslavskii map

Chaos systems	Bouncing ball dynamics Chua's circuit Economic bubble Tilt-A-Whirl

Chaos theorists	Michael Berry Leon O. Chua Mitchell Feigenbaum Martin Gutzwiller Brosl Hasslacher Michel Hénon Edward Norton Lorenz Aleksandr Lyapunov Benoît Mandelbrot Henri Poincaré Otto Rössler David Ruelle Oleksandr Mykolaiovych Sharkovsky Floris Takens James A. Yorke

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