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Ikeda map : ウィキペディア英語版
Ikeda map

In physics and mathematics, the Ikeda map is a discrete-time dynamical system given by the complex map
: z_ = A + B z_n e^
The original map was proposed first by Ikeda as a model of light going around
across a nonlinear optical resonator (ring cavity containing a nonlinear dielectric medium) in a more general form. It is reduced to the above simplified "normal" form by Ikeda, Daido and Akimoto 〔K.Ikeda,
Multiple-valued Stationary State and its Instability of the Transmitted Light by a Ring Cavity System, Opt. Commun. 30 257-261 (1979); K. Ikeda, H. Daido and O. Akimoto, Optical Turbulence: Chaotic Behavior of Transmitted Light from a Ring Cavity, Phys. Rev. Lett. 45, 709–712 (1980)〕 z_n stands for the electric field inside the resonator at the n-th step of rotation in the resonator, and A and C are parameters which indicates laser light applied from the outside, and linear phase across the resonator, respectively. In particular
the parameter B \leq 1 is called dissipation parameter characterizing
the loss of resonator, and in the limit of B=1 the Ikeda map becomes
a conservative map.
The original Ikeda map is often used in another modified form in order
to take the saturation effect of nonlinear dielectric medium into account:
: z_ = A + B z_n e^
A 2D real example of the above form is:
: x_ = 1 + u (x_n \cos t_n - y_n \sin t_n), \,
: y_ = u (x_n \sin t_n + y_n \cos t_n), \,
where ''u'' is a parameter and
: t_n = 0.4 - \frac.
For u \geq 0.6, this system has a chaotic attractor.
==Attractor==
This animation shows how the attractor of the system changes as the parameter u is varied from 0.0 to 1.0 in steps of 0.01. The Ikeda dynamical system is simulated for 500 steps, starting from 20000 randomly placed starting points. The last 20 points of each trajectory are plotted to depict the attractor. Note the bifurcation of attractor points as u is increased.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「Ikeda map」の詳細全文を読む



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