emergence of coherence and scaling in an ensemble of globally coupled chaotic systems
DESCRIPTION
Emergence of Coherence and Scaling in an Ensemble of Globally Coupled Chaotic Systems. Sang-Yoon Kim Department of Physics Kangwon National University. Globally Coupled Systems (Each element is coupled to all the other ones with equal strength). Synchronized Flashing of Fireflies. - PowerPoint PPT PresentationTRANSCRIPT
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Emergence of Coherence and Scaling in an Ensemble of Globally Coupled Chaotic Systems
Sang-Yoon Kim
Department of Physics
Kangwon National University
Globally Coupled Systems (Each element is coupled to all the other ones with equal strength)
Biological Examples Heartbeats, Circadian Rhythms, Brain Rhythms, Flashing of Fireflies
Nonbiological Examples Josephson Junction Array, Multimode Laser, Electrochemical Oscillator
Incoherent State
(i: index for the element, : Ensemble Average)
(each element’s motion: independent) (collective motion)Coherent State
Stationary Snapshots Nonstationary Snapshots
t = n t = n+1
Synchronized Flashing of Fireflies
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Emergent Science
“The Whole is Greater than the Sum of the Parts.”
Complex Nonlinear Systems: Spontaneous Emergence of Dynamical Order
Order Parameter ~ 0 Order Parameter < 1 Order Parameter ~ 1
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Two Mechanisms for Synchronous Rhythms
Leading by a Pacemaker Collective Behavior of All Participants
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Synchronization of Pendulum Clocks
Synchronization by Weak Coupling Transmitted through the Air or by Vibrations in the Wall to which Theyare Attached
First Observation of Synchronization by Huygens in Feb., 1665
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Circadian Rhythms
Biological Clock Ensemble of Neurons in the Suprachiasmatic Nuclei (SCN) Located within the Hypothalamus: Synchronization → Circadian Pacemaker
[Zeitgebers (“time givers”): light/dark]
Time of day (h) Time of day (h)
Tem
pera
ture
(ºc
)
Gro
wth
Hor
mon
e (n
g/m
L)
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Integrate and Fire (Relaxation) Oscillator Mechanical Model for the IF Oscillator
Van der Pol (Relaxation) Oscillator
Accumulation (Integration) “Firing”
wat
er le
vel
wat
er o
utfl
ow
time
time
Neuron Firings of a Neuron Firings of a Pacemaker Cell in the Heart
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Synchronization in Pulse-Coupled IF Oscillators
Population of Globally Pulse-Coupled IF Oscillators
)(any for )N
min(1,:Coupling Pulse
ResettingFiring: of Value Threshold
ij(t)x)t(x)t(x
vv
.N,...,i,v,Ivdtdv
jii
ii
iii
1
01
110
Full Synchronization
Kicking
Heart Beat: Stimulated by the Sinoatrial (SN) Node Located on the Right Atrium, Consisting of Pacemaker Cells 410
20
2
.
I
[R. Mirollo and S. Strogatz, SIAM J. Appl. Math. 50, 1645 (1990)]
[Lapicque, J. Physiol. Pathol. Gen. 9, 620 (1971)]
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Emergence of Dynamical Order and Scaling in A Large Population of Globally Coupled Chaotic Systems
Scaling Associated with Coherence with a Macroscopic
Mean Field Successive Appearance of Similar
Coherent States of Higher Order
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99
Period-Doubling Route to Chaos
Lorenz Attractor[Lorenz, J. Atmos. Sci. 20, 130 (1963)]
Butterfly Effect [Small Cause Large Effect] Sensitive Dependence on Initial Conditions
Logistic Map[May, Nature 261, 459 (1976)]
21 1)( ttt axxfx : Representative Model for Period-Doubling Systems
a*a
: Lyapunov Exponent (exponential divergence rate of nearby orbits) 0 Regular Attractor > 0 Chaotic Attractor
a*a
Transition to Chaos at a Critical Point a* (=1.401 155 189 …) via an Infinite Sequence of Period Doublings
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Universal Scaling Associated with Period Doublings Noisy Logistic Map
;)(1 ttt xfx
Parametrically Forced Pendulum
[ M.J. Feigenbaum, J. Stat. Phys. 19, 25 (1978), J. Crutchfield, M. Nauenberg, and J. Rudnick, Phys. Rev. Lett. 46, 459 (1981). B. Shraiman, C.E. Wayne, and P.C. Martine, Phys. Rev. Lett. 46, 462 (1981).]
nce.unit varia a andmean zero a with noise random uniform :)(
strength, noise:
t
310 /10 3 Universal Scaling Factors: =4.669 201 … =-2.502 987 … =6.619 03
w: Gaussian White Noise with <w(t)>=0 and <w(t1) w(t2)> = (t1 – t2).
.2sin)2cos(22),,(),),,(, 211111 xtAytyxfttyxfyyx w
[S.-Y. Kim and K. Lee, Phys. Rev. E 53, 1579 (1996).]
-A*
h(t)=Acos(2t)
(=2, =1, A* = 6.57615 …)
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Globally Coupled Noisy Chaotic Systems
An Ensemble of Globally Coupled Noisy Logistic Maps
....,,1];))(())((1
[)())(()1(1
NitxftxfN
ttxftx i
N
jjiii
• A Population of 1D Chaotic Maps Interacting via the Mean Field:
N
jjj txf
Ntxfth
1
))((1
))(()(
:
:)t(;ax)x(f
21
• Dissipative Coupling Tending to Equalize the States of Elements
Investigation: Coherence in Asynchronous Chaotic Attractors and Scaling Associated with the Mean Field
Uniform Random Noise with a Zero Mean and Unit Variance
Parameter to Control the Noise Strength
Main Interest
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Scaling near the Zero-Coupling Critical Point (N=10 ) Universal Scaling near the Zero-Coupling Critical Point (a, , ) = (a*, 0, 0): (a* = 1.401 155 189 …)
Dynamical Behavior at a Set of Parameters (a, , ) Dynamical Behavior [with Doubled Time Scale (t=2)] at a Set of Renormalized Parameters (a/, / c, /) [=4.669201, =6.61903]
Asynchronous Chaotic Attractors (containing the diagonal)
“Scaling Factor for the Coupling Parameter for the Dissipative Coupling:
/.
,/.,/.a
0010
2020320
0010
020320
.
,.,.a
2
22
0010
2020320
/.
,/.,/.a
[ Renormalization Results: 1. S.P.Kuznetsov, Radiophysics and Quantum Electronics 28, 681 (1985). 2. S.-Y. Kim and H. Kook, Phys. Rev. E 48, 785 (1993). 3. S.-Y. Kim and H. Kook, Phys. Lett. A 178, 258 (1993).]
2c
4
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Ensemble-Averaged Mean Field h(t)
)(ofAverageTime:)(1
lim)(,1
)(1
T1
ththT
th(t))f(xN
thT
t
n
jj
ary)Nonstation(
)Stationary:(
:h(t))t(h)t(h
)t(h)t(h)t(h
In the Thermodynamic Limit of N→∞,
Coherent and Incoherent States
Incoherent State (Each Element: Independent Motion)
Coherent State (Collective Motion)
Multiple Transitions to Coherence for 0010320104 ..aN and,,
Incoherent State (Gray, ε=0.02)Coherent State (Black, ε=0.03)
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Mean- Field Dynamic of Asynchronous Chaotic Attractors for Δa=0.32
ε=0.02 ε=0.03 ε=0.03
ε=0.033 ε=0.035 ε=0.036
ε=0.036ε=0.035ε=0.033
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Order Parameter for the Coherent Transition
Order Parameter
:))()(())(( 22 ththth Variance (Mean Square Deviation) of the Mean Field h(t)
In the Thermodynamic Limit of N→∞, > 0 for the Coherent State → 0 for the Incoherent State
∆a=0.32,σ=0.001
ε
ε*~0.0291
∆
εIncoherent State Coherent State
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Scaling for the Mean Field
N
jj txf
Nth
1
))((1
)(Mean Field : Exhibiting the ‘2’-scaling (=-2.502 987 …)
Return Maps of the Mean Field for
a=0.32/i, =0.02/2i, =0.001/i, t =2i
[i (level of renormalization)=0, 1, 2]
Orbital Scalings in the Logistic Map
‘’-scaling near the Critical Point x=0
‘2’-scaling near the First Iterate of the Critical Point x=1 [= f(0)]
1)t(hi increases, level theAs
410N
21 1 tt axx
x=1 (most concentrated region)
x=0 (most rarified region)
1
2
1
) h(2i
h(2
τ+
1))
τ
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Appearance of Similar Coherent States of Higher Orders (N=10 )
1st-Order Renormalized State (a=0.32/, =0.001/)
2nd-Order Renormalized State (a=0.32/2, =0.001/2)
3rd-Order Renormalized State (a=0.32/3, =0.001/3)
=0.039/23
=0.039/22
=0.039/2
Bifurcation Diagram Variance Diagram Return Map
4
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Self-Similar State Diagrams (N=10 )
Incoherent States (White)Coherent States (Gray)
1st Renormalized State Diagram 2nd Renormalized State Diagram=0.001/ =0.001/2
=0.001
4
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Effect of Noise on the Transition to Coherence
Scaling for the State Diagram in the - Plane
Multiple Transitions to Coherence for < * (=0.003)
Single Period-Doubling Transition to Coherence for > *
1st Order Renormalized State Diagram
a=0.32/
2nd Order Renormalized State Diagram
0th Order State Diagram
a=0.32/2
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A Global Population of Inertially Coupled Maps
....,,1),...,,,()())(()1(11
Nixxxgttxftxiiiiii
Renormalization Result for the Scaling of the Coupling Parameter:
Nonlinear Coupling [Tendency of equalizing the states of the elements Dissipative coupling]
coupling quadratic :))(())((1
)...,,,( :e.g.1
11 txftxfN
xxxg i
N
jjiii
Linear Coupling
One Relevant Scaling Factor: =2
)()(1
)...,,,(1
11 txtxN
xxxg i
N
jjiii
Two Relevant Scaling Factors:
1 = (=-2.502 987 …): inertial coupling (each element: maintaining the memory of its previous states)
Combination of the Linear and Quadratic Coupling
Pure Inertial Coupling with Only One Relevant Scaling Factor: =
))](())((1
[088.0)]()(1
[)...,,,(11
11 txftxfN
txtxN
xxxg i
N
jji
N
jjiii
[Ref: S.P. Kuznetsov, Chaos, Solitons, and Fractals 2, 281-301 (1992).]
[Renormalization Results: S.P.Kuznetsov, Radiophysics and Quantum Electronics 28, 681 (1985). S.-Y. Kim and H. Kook, Phys. Rev. E 48, 785 (1993). S.-Y. Kim and H. Kook, Phys. Lett. A 178, 258 (1993).]
2 = 2
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Scaling near the Zero-Coupling Critical Point (N=10 ) Universal Scaling near the Zero-Coupling Critical Point (a, , ) = (a*, 0, 0): (a* = 1.401 155 189 …)
Dynamical Behavior at a Set of Parameters (a, , ) Dynamical Behavior [with Doubled Time Scale (t=2)] at a Set of Renormalized Parameters (a/, / c, /) [=4.669201, =6.61903]
Asynchronous Chaotic Attractors (containing the diagonal)
“Scaling Factor for the Coupling Parameter for the Inertial Coupling:
/.
,/.,/.a
0030
020320
0030
020320
.
,.,.a
2
22
0030
020320
/.
,/.,/.a
[ Renormalization Results: 1. S.P.Kuznetsov, Radiophysics and Quantum Electronics 28, 681 (1985). 2. S.-Y. Kim and H. Kook, Phys. Rev. E 48, 785 (1993). 3. S.-Y. Kim and H. Kook, Phys. Lett. A 178, 258 (1993).]
)5029872( ....c
4
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Onset of Coherence
Bifurcation Diagram and Return Map of the Mean Field k(t) (N=10 )
N
j
T
tT
j tktktΔk,tkT
tk,txN
tk1
)()()()(1
lim)()(1
)(
)( FieldMean theof Variance:))()(())(( 22 tktktktk
Order Parameter
0340.*r
0070.*
l
Δa=0.32σ=0.003
Coherent Incoherent Coherent
4
Coherent State for ε=0.04Incoherent State for ε=0.02
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Scaling for the Mean Field
N
jj tx
Ntk
1
)(1
)(Mean Field : Exhibiting the ‘’-scaling (=-2.502 987 …)
Return Maps of the Mean Field for
a=0.32/i, =0.02/2i, =0.003/i, t =2i
[i (level of renormalization)=0, 1, 2]
Orbital Scalings in the Logistic Map
‘’-scaling near the Critical Point x=0
0)(increases, level theAs tki
410N
21 1 tt axx
x=1 (most concentrated region)
x=0 (most rarified region)
1
2
1
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Scaling Associated with the Mean Field k(t) (N=10 )
1st-Order Renormalized State (a=0.32, =0.003)
2nd-Order Renormalized State (a=0.32/, =0.003/)
3rd-Order Renormalized State (a=0.32/2, =0.003/2)
=0.04/2
=0.04/
=0.04
Bifurcation Diagram Variance Diagram Return Map
N
jj
txN
tk1
)(1
)( :FieldMean
4
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Coherence and Scaling in a Heterogeneous Ensemble ofGlobally Coupled Maps
Heterogeneous Ensemble (consisting of non-identical elements)
....,,1,)),(()),((1
)),(()1(1
NiatxfatxfN
atxftx ii
N
jjjiii
Spread in the map parameter ai for each element: Randomly chosen with uniform distribution in the interval of (a-, a+) (: spread parameter)
Transition from an Incoherent to a Coherent State
N
jj txf
Nth
1
))((1
)( :FieldMean
Occurrence of a Coherence at =* (=0.0289) for a=0.32 and =0.006 Coherent State for =0.03Incoherent State for ε=0.02
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Return Map
Successive Appearance of Similar Coherent States of Higher Orders
1st-Order Renormalized State (a=0.32/, =0.006/)
2nd-Order Renormalized State (a=0.32/2, =0.006/2)
3rd-Order Renormalized State (a=0.32/3, =0.006/3)
Bifurcation Diagram Variance Diagram
=0.038/2
=0.038/22
=0.038/23
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An Ensemble of Globally Coupled Noisy Pendulums Globally Coupled Noisy Pendulums
Phase Coherent Attractor in the Single Pendulum
.2sin)2cos(22),,(],1
[),,(, 2
1
xtAytyxfyyN
tyxfyyx i
N
jjiiiiii
strength. Noise :),()()(n correlatio delta and 0mean zero a with noise hiteGaussian w : 2121 tttt
)(
)(tan 1
tx
ty
22 yx
yxyx
...),,n(
nf||
21
2
at peaks
N
jj
N
jj
tyN
tYtxN
tX11
)(1
)(,)(1
)(A=0.06=0.0015=0.2
=2, =1A(A-A*)=0.06 (A*=6.57615)=0.0015
Phase Coherence (Flow) and Amplitude Incoherence
• Mean Field: Rotation on a Noisy Limit Cycle (Flow), Noisy Stationary State (Map)
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Onset of Coherence
Bifurcation Diagram and Return Map of the Mean Field H(n) (N=10 )
)n(H))n(H)n(H())n(H( theof Variance:22
Order Parameter
33670.*r
Incoherent Coherent
4
Coherent State for ε=0.04Incoherent State for ε=0.02
N
jj )n(y
N)n(H
1
1 :FieldMean
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1st-Order Renormalized State (A=0.06/, =0.0015/)
2nd-Order Renormalized State (A=0.06/2, =0.0015/2)
3rd-Order Renormalized State (A=0.06/3, =0.0015/3)
Scaling Associated with the Mean Field H(n) (N=10 )4
=0.3/2
=0.3/22
=0.3/23
Return MapMSD DiagramBifurcation Diagram
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Summary
Investigation of Onset of Coherence in an Ensemble of Globally Coupled Noisy Logistic Maps
Universality for the Results
Confirmed in a Population of Globally Coupled Noisy Pendulums
(a, , ) (a*, 0, 0): zero-coupling critical point
Successive Appearance of Similar Coherent States of Higher Orders
Our Results: Valid in an Ensemble of Globally Coupled Period-Doubling Systems of Different Nature