We consider systems of many spatially distributed phase oscillators that interact with their neighbors. Each oscillator is allowed to have a different natural frequency, as well as a different response time to the signals it receives from other oscillators in its neighborhood. Using the ansatz of Ott and Antonsen [Chaos 18, 037113 (2008)] and adopting a strategy similar to that employed in the recent work of Laing [Physica D 238, 1569 (2009)], we reduce the microscopic dynamics of these systems to a macroscopic partial-differential-equation description. Using this macroscopic formulation, we numerically find that finite oscillator response time leads to interesting spatiotemporal dynamical behaviors including propagating fronts, spots, target patterns, chimerae, spiral waves, etc., and we study interactions and evolutionary behaviors of these spatiotemporal patterns.

1.
A.
Pikovsky
,
M.
Rosenblum
, and
J.
Kurths
,
Synchronization: A Universal Concept in Nonlinear Sciences
(
Cambridge University Press
,
Cambridge
,
2004
).
2.
S.
Strogatz
,
Sync: The Emerging Science of Spontaneous Order
(
Hyperion
,
New York
,
2003
).
3.
A. T.
Winfree
,
The Geometry of Biological Time
, 2nd ed. (
Springer
,
Berlin
,
2001
).
4.
J.
Buck
,
Q. Rev. Biol.
63
,
265
(
1988
).
5.
S. H.
Strogatz
,
D. M.
Abrams
,
A.
McRobie
,
B.
Eckhardt
, and
E.
Ott
,
Nature
438
,
43
(
2005
).
6.
L.
Glass
and
M. C.
Mackey
,
From Clocks to Chaos: The Rhythms of Life
(
Princeton University Press
,
New Jersey
,
1988
).
7.
T. D.
Frank
,
A.
Daffertshofer
,
C. E.
Peper
,
P. J.
Beek
, and
H.
Haken
,
Physica D
144
,
62
(
2000
).
8.
J.
Garcia-Ojalvo
,
M. B.
Elowitz
, and
S. H.
Strogatz
,
Proc. Natl. Acad. Sci.
101
,
10955
(
2004
).
9.
T.
Matsuo
,
S.
Yamaguchi
,
S.
Mitsui
,
A.
Emi
,
F.
Shimoda
, and
H.
Okamura
,
Science
302
,
255
(
2003
).
10.
Y.
Kuramoto
,
Chemical Oscillations, Waves, and Turbulence
(
Dover
,
New York
,
1984
).
11.
I. Z.
Kiss
,
Y.
Zhai
, and
J. L.
Hudson
,
Science
296
,
1676
(
2002
).
12.
A. F.
Taylor
,
M. R.
Tinsley
,
F.
Wang
,
Z.
Huang
, and
K.
Showalter
,
Science
323
,
614
(
2009
).
13.
H.
Hong
,
M. Y.
Choi
, and
B. J.
Kim
,
Phys. Rev. E
65
,
026139
(
2002
).
14.
T.
Ichinomiya
,
Phys. Rev. E
70
,
026116
(
2004
).
15.
Y.
Moreno
and
A. F.
Pacheco
,
Europhys. Lett.
68
,
603
(
2004
).
16.
J. G.
Restrepo
,
E.
Ott
, and
B. R.
Hunt
,
Chaos
16
,
015107
(
2005
).
17.
Y.
Kuramoto
and
D.
Battogtokh
,
Nonlinear Phenom. Complex Syst.
5
,
380
(
2002
).
18.
S.
Shima
and
Y.
Kuramoto
,
Phys. Rev. E
69
,
036213
(
2004
).
19.
D. A.
Abrams
and
S. H.
Strogatz
,
Int. J. Bifurcation Chaos
16
,
21
(
2006
).
20.
21.
M. K. S.
Yeung
and
S. H.
Strogatz
,
Phys. Rev. Lett.
82
,
648
(
1999
).
22.
M. Y.
Choi
,
H. J.
Kim
,
D.
Kim
, and
H.
Hong
,
Phys. Rev. E
61
,
371
(
2000
).
23.
W. S.
Lee
,
E.
Ott
, and
T. M.
Antonsen
,
Phys. Rev. Lett.
103
,
044101
(
2009
).
24.
E.
Ott
and
T. M.
Antonsen
,
Chaos
18
,
037113
(
2008
).
25.
E.
Ott
and
T. M.
Antonsen
,
Chaos
19
,
023117
(
2009
).
26.
E.
Ott
,
B.
Hunt
, and
T. M.
Antonsen
, e-print arXiv:1005.3319, Chaos (to be published).
27.
We note that the general method of Refs. 24–26 has also been widely applied to a variety of problems involving large coupled systems of phase oscillators. Some examples are the following:
L. M.
Alonso
and
G. B.
Mindlin
,
Chaos
21
,
023102
(
2011
);
[PubMed]
A.
Ghosh
,
D.
Roy
, and
V. K.
Jirsa
,
Phys. Rev. E
80
,
041930
(
2009
);
M. M.
Abdulrehem
and
E.
Ott
,
Chaos
19
,
013129
(
2009
);
[PubMed]
L. M.
Childs
and
S. H.
Strogatz
,
Chaos
18
,
043128
(
2008
);
[PubMed]
S. A.
Marvel
and
S. H.
Strogatz
,
Chaos
19
,
013132
(
2009
);
[PubMed]
L. F.
Lafuerza
,
P.
Colet
, and
R.
Toral
,
Phys. Rev. Lett.
105
,
084101
(
2010
);
[PubMed]
K. H.
Nagai
and
H.
Kori
,
Phys. Rev. E
81
,
065202
(
2010
);
E. A.
Martens
,
E.
Barreto
,
S. H.
Strogatz
,
E.
Ott
,
P.
So
, and
T. M.
Antonsen
,
Phys. Rev. E
79
,
026204
(
2009
);
D.
Pazó
and
E.
Montbrió
,
Phys. Rev. E
80
,
046215
(
2009
);
Z.
Levajic
and
A.
Pikovsky
,
Phys. Rev. E
82
,
056202
(
2010
);
P.
So
,
B. C.
Cotton
and
E.
Barreto
,
Chaos
18
,
037114
(
2008
);
[PubMed]
Y.
Kawamura
,
H.
Nakao
,
K.
Arai
,
H.
Kori
, and
Y.
Kuramoto
,
Chaos
20
,
043110
(
2010
);
[PubMed]
A.
Pikovsky
and
M.
Rosenblum
,
Phys. Rev. Lett.
101
,
264103
(
2008
);
[PubMed]
C. R.
Laing
,
Chaos
19
,
013113
(
2009
);
[PubMed]
E. A.
Martens
,
Phys. Rev. E
82
,
016216
(
2010
);
G.
Bordyugov
,
A.
Pikovsky
, and
M.
Rosenblum
,
Phys. Rev. E
82
,
035205
(
2010
);
E. A.
Martens
,
Chaos
20
,
043122
(
2010
);
[PubMed]
H.
Hong
and
S. H.
Strogatz
,
Phys. Rev. Lett.
106
,
054102
(
2011
).
[PubMed]
28.
G. C.
Sethia
and
A.
Sen
,
Phys. Rev. Lett.
100
,
144102
(
2008
).
29.
Like some previous models, our system, Eqs. (27)–(29), has the general form of a complex Ginzburg-Landau equation [cf. Eq. (27)] with nonlocal coupling [cf. Eq. (29)]. For example, see
D.
Tanaka
and
Y.
Kuramoto
,
Phys. Rev. E
68
,
026219
(
2003
).
30.
S.
Chapman
and
T. G.
Cowling
,
The Mathematical Theory of Non-uniform Gases
(
Cambridge University Press
,
Cambridge
,
1952
).
31.
I. S.
Aranson
and
L.
Kramer
,
Rev. Mod. Phys.
74
,
99
(
2002
).
32.
H.
Mori
and
Y.
Kuramoto
,
Dissipative Structures and Chaos
(
Springer
,
Berlin
,
1998
).
33.
E. A.
Martens
,
C. R.
Laing
, and
S. H.
Strogatz
,
Phys. Rev. Lett
104
,
044101
(
2010
).
34.
Y.
Kuramoto
,
S.
Shima
,
D.
Battogtokh
, and
Y.
Shiogai
,
Prog. Theor. Phys. Suppl.
161
,
127
(
2006
).
35.
R. J.
Deissler
and
H. R.
Brand
,
Phy. Rev. Lett.
72
,
478
(
1994
).
36.
N.
Akhmediev
,
J. M.
Soto-Crespo
, and
G.
Town
,
Phy. Rev. E
63
,
056602
(
2001
).
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