xt+1 = 1.0 + μ (xt cosθt - yt sinθt)
yt+1 = μ (xt sinθt + yt cosθt)
θt = a - b/(1.0 + xt2 + yt2)
case 1
parameters: μ = 0.9, a = 0.4, b = 6.0
Lyapunov exponents (log with base-e): 0.50752, -0.71824
Lyapunov Dimension: 1.7066
The sum of the Lyapunov exponents is theoretically the same as 2 ln(μ).
case 2
parameters: μ = 0.83, a = 0.4, b = 6.0
Lyapunov exponents (log with base-e): 0.39272, -0.76538
Lyapunov Dimension: 1.5131
The sum of the Lyapunov exponents is theoretically the same as 2 ln(μ).
Reference
Multiple-valued stationary state and its instability of the transmitted light by a ring cavity system
Kensuke Ikeda
Optics Communications, 30, 257–261 (1979)
DOI: 10.1016/0030-4018(79)90090-7
Computing the Lyapunov spectrum of a dynamical system from an observed time series
Reggie Brown, Paul Bryant, and Henry Don Isaac Abarbanel
Physical Review A 43, 2787-2806 (1991)
Chaos and Time-Series Analysis (p. 424)
Julien Clinton Sprott
Oxford University Press (2001/Sep/27)
ISBN-10: 0198508409
ISBN-13: 978-0198508403
programme
ikeda_lyap.c contains the main function.
case 1
case 2