Following a short report of our preliminary results [Phys. Rev. E 79, 055203(R) (2009)], we present a more detailed study of the effects of coupling delay in diffusively coupled phase oscillator populations. We find that coupling delay induces chimera and globally clustered chimera (GCC) states in delay coupled populations. We show the existence of multi-clustered states that act as link between the chimera and the GCC states. A stable GCC state goes through a variety of GCC states, namely periodic, aperiodic, long-- and short--period breathers and becomes unstable GCC leading to global synchronization in the system, on increasing time delay. We provide numerical evidence and theoretical explanations for the above results and discuss possible applications of the observed phenomena.
Deep Dive into Chimera and globally clustered chimera: Impact of time delay.
Following a short report of our preliminary results [Phys. Rev. E 79, 055203(R) (2009)], we present a more detailed study of the effects of coupling delay in diffusively coupled phase oscillator populations. We find that coupling delay induces chimera and globally clustered chimera (GCC) states in delay coupled populations. We show the existence of multi-clustered states that act as link between the chimera and the GCC states. A stable GCC state goes through a variety of GCC states, namely periodic, aperiodic, long– and short–period breathers and becomes unstable GCC leading to global synchronization in the system, on increasing time delay. We provide numerical evidence and theoretical explanations for the above results and discuss possible applications of the observed phenomena.
arXiv:1003.4345v1 [nlin.AO] 23 Mar 2010
Chimera and globally clustered chimera: Impact of time delay
Jane H. Sheeba,1 V. K. Chandrasekar,1 and M. Lakshmanan1
1Centre for Nonlinear Dynamics, School of Physics,
Bharathidasan University, Tiruchirappalli - 620 024, Tamilnadu, India
Following a short report of our preliminary results [Phys. Rev. E 79, 055203(R) (2009)], we
present a more detailed study of the effects of coupling delay in diffusively coupled phase oscillator
populations. We find that coupling delay induces chimera and globally clustered chimera (GCC)
states in delay coupled populations. We show the existence of multi-clustered states that act as
link between the chimera and the GCC states. A stable GCC state goes through a variety of GCC
states, namely periodic, aperiodic, long– and short–period breathers and becomes unstable GCC
leading to global synchronization in the system, on increasing time delay. We provide numerical
evidence and theoretical explanations for the above results and discuss possible applications of the
observed phenomena.
PACS numbers: 05.45.Xt, 2.30.Ks, 89.75.-k, 87.85.dq
I.
INTRODUCTION
Kuramoto, Battogokh and Shima discovered [1–3]
an interesting spatiotemporal pattern which was later
named chimera by Abrams and Strogatz [4, 5].
The
name chimera, which literally refers to something that
is composed of seemingly incompatible or incongruous
parts, was coined for this phenomenon because a group of
identical oscillators splits into two groups of completely
different character.
Since its discovery [1, 2, 4], vari-
ous theoretical and numerical developments have been
reported on the stability of chimera states and their ex-
istence in systems with varied structures [4, 6], including
time delay [7]. It is clear that the chimera state cannot be
attributed to partial synchronization. The occurrence of
partial synchronization in a population of non-identical
oscillators is not surprising. On the other hand, if an
identical group of oscillators splits into synchronized and
desynchronized groups, it is called chimera. Therefore,
the discovery of chimera came as a surprise in the study
of synchronization phenomenon in complex systems.
By and large, synchronization in coupled oscillator sys-
tems has been analytically and numerically investigated
in a rigorous manner over the past years [9, 10]. Possible
routes to global synchronization and methods to control
synchronization have also been proposed [11, 12]. How-
ever, complete understanding of the effects induced by
coupling delay in synchronization of coupled oscillator
systems is still an open problem. It is well known that
time delay occurs in real physical systems. For example,
in a network of neuronal populations, there is certainly
a significant delay in propagation of signals. In addition
there can also be synaptic and dendritic delays. Other
examples include finite reaction times of chemicals and fi-
nite transfer times associated with the basic mechanisms
that regulate gene transcription and mRNA translation.
The nature of coupling in coupled oscillator systems
has been conventionally considered as instantaneous dur-
ing earlier studies. One of the main reasons for this as-
sumption is that it substantially simplifies the analysis of
0
50
100
0
3
6
t
θi
(1,2)
Chimera
0
100
200
0
3
6
Globally clustered chimera
FIG. 1: (Color online) Occurrence of stable chimera and GCC
states in system (1). Black and green (grey) lines represent os-
cillators in the first and the second populations, respectively.
Here {f, h} = {sin(θ), cos(θ)}, τ1 = nτ2 = nτ with n = 0,
A = 0.4, B = 0.6 and τ = 2 for the chimera and τ = 4 for the
GCC.
the system. In addition, such an approximation is more
often physically justified. However, the fact is that the
consideration of time delay is vital for modeling real life
systems. Furthermore, as we will demonstrate in this pa-
per, certain interesting dynamical phenomena in complex
systems are characteristic of time delay and they will not
occur in systems without time delay.
Since the intro-
duction of time delay increases the effective dimension of
the system, one can expect certain complex phenomena
to be explained in a better way in models of real physical
systems when delay is included.
In this paper, following our Rapid Communication [13],
we present a more detailed discussion of the effects of
coupling delay in inducing chimera and globally clus-
tered chimera (GCC) states in systems of coupled iden-
tical oscillator populations.
By a GCC state, here we
mean a state where the system splits into two different
groups, one synchronized and the other desynchronized,
each group comprised of oscillators from both the popu-
lations. Since a global clustering (mixing) of oscillators
from both the populations occur in this case, we call this
state a GCC. This is different from the chimera state
2
Population−I
Population−II
FIG. 2: Schematic representation of system (1) with N = 3
comprised of two populations of all–to–all cou
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