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Quasiperiodicity & Mode Locking in The Circle Map
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Quasiperiodicity & Mode Locking in The Circle Map
Lyapunov exponent
Circle map
Eui-Sun Lee
Department of Physics
Kangwon National University
.1mod,)θ π 2 sin(π2
θ)θ(θ nnn1n
Kf
.|)θ('|ln1
limσ1
0j
t
jt
ft
Winding number
.n
θθlimK),W( 0n
n
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Phase Diagram in The Circle Map
Gray No. irrational:W0,σ:statedicQuasiperioWhite 0σ:stateChaotic
Black No. rational : W0, σ :state Periodic
• The regions the (Ω,K) where W occupies rational values, are called Arnold Tongues.
2/)15(W :No. ngmean windi-golden having state dicquasiperio of )Wpath(The
1/2 2/3
1/13/43/5 4/5 5/65/7
W
4/7
• has the 1D structure, and then ends at the critical point (K=1).W
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Devil’s Staircase In the subcritical region(0<K<1), the plot of W vs. Ω show the devils staircase.
3
1
4
12
1
1
0
1
0
4
1 3
12
1
1
0
The winding No. is locked in at every single rational No. in a nonzero interval of Ω,and the plateaus exist densely.
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1
3
1
4
1
1
0
5
1
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Measure of Mode locking
As K Increases toward 1 from 0 in The Subcritical Region, The Measure(M) of The Mode-locked State Increases Monotonically.
Near ΔK(=1-K) decreases, 1-M exhibits the power law scaling, 1-M~ΔK β
,where β = 0.305 ± 0.004 .
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Bifurcation Structure in the Arnold Tongues
Swallow tail structure in the Arnold tongue exhibit self-similarity, and period-doubling transition to chaos occurs
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Summary
1. The region in the (Ω,K) space where winding No. of the periodic state is locked in a single rational No., is called Arnold Tongues.
2. The inverse of golden-mean quasiperiodic state path has the 1D structure, and then ends at the critical point (K=1).
3. As K increases toward1 from 0 in the subcritical region, the measure(M) of the mode-locked state increases monotonically.
4. Swallow tail structure in the Arnold tongue exhibit self-similarity, and period-doubling transition to chaos occurs.