Transcritical riddling in a system of coupled maps

被引:19
作者
Popovych, O [1 ]
Maistrenko, Y
Mosekilde, E
Pikovsky, A
Kurths, J
机构
[1] Natl Acad Sci Ukraine, Inst Math, UA-01601 Kiev, Ukraine
[2] Tech Univ Denmark, Dept Phys, DK-2800 Lyngby, Denmark
[3] Univ Potsdam, Dept Phys, PF 601553, D-14415 Potsdam, Germany
关键词
D O I
10.1103/PhysRevE.63.036201
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
The transition from fully synchronized behavior to two-cluster dynamics is investigated for a system of N globally coupled chaotic oscillators by means of a model of two coupled logistic maps. An uneven distribution of oscillators between the two clusters causes an asymmetry to arise in the coupling of the model system. While the transverse period-doubling bifurcation remains essentially unaffected by this asymmetry, the transverse pitchfork bifurcation is turned into a saddle-node bifurcation followed by a transcritical riddling bifurcation in which a periodic orbit embedded in the synchronized chaotic state loses its transverse stability. We show that the transcritical riddling transition is always hard. For this, we study the sequence of bifurcations that the asynchronous point cycles produced in the saddle-node bifurcation undergo, and show how the manifolds of these cycles control the magnitude of asynchronous bursts. In the case where the system involves two subpopulations of oscillators with a small mismatch of the parameters, the transcritical riddling will be replaced by two subsequent saddle-node bifurcations, or the saddle cycle involved in the transverse destabilization of the synchronized chaotic state may smoothly shift away from the synchronization manifold. In this way, the transcritical riddling bifurcation is substituted by a symmetry-breaking bifurcation, which is accompanied by the destruction of a thin invariant region around the symmetrical chaotic state.
引用
收藏
页数:15
相关论文
共 62 条
[1]   RIDDLED BASINS [J].
Alexander, J. C. ;
Yorke, James A. ;
You, Zhiping ;
Kan, I. .
INTERNATIONAL JOURNAL OF BIFURCATION AND CHAOS, 1992, 2 (04) :795-813
[2]  
ARNOLD VI, 1978, THEORY ORDINARY DI 2
[3]   On riddling and weak attractors [J].
Ashwin, P ;
Terry, JR .
PHYSICA D-NONLINEAR PHENOMENA, 2000, 142 (1-2) :87-100
[4]   On the unfolding of a blowout bifurcation [J].
Ashwin, P ;
Aston, PJ ;
Nicol, M .
PHYSICA D, 1998, 111 (1-4) :81-95
[5]   From attractor to chaotic saddle: A tale of transverse instability [J].
Ashwin, P ;
Buescu, J ;
Stewart, I .
NONLINEARITY, 1996, 9 (03) :703-737
[6]   Loss of chaos synchronization through the sequence of bifurcations of saddle periodic orbits [J].
Astakhov, V ;
Shabunin, A ;
Kapitaniak, T ;
Anishchenko, V .
PHYSICAL REVIEW LETTERS, 1997, 79 (06) :1014-1017
[7]   Effect of parameter mismatch on the mechanism of chaos synchronization loss in coupled systems [J].
Astakhov, V ;
Hasler, M ;
Kapitaniak, T ;
Shabunin, A ;
Anishchenko, V .
PHYSICAL REVIEW E, 1998, 58 (05) :5620-5628
[8]   PARALLEL COMPUTER-SIMULATION OF NEAREST-NEIGHBOUR INTERACTION IN A SYSTEM OF NEPHRONS [J].
BOHR, H ;
JENSEN, KS ;
PETERSEN, T ;
RATHJEN, B ;
MOSEKILDE, E ;
HOLSTEINRATHLOU, NH .
PARALLEL COMPUTING, 1989, 12 (01) :113-120
[9]   DISCRETE-TIME POPULATION-DYNAMICS OF INTERACTING SELF-OSCILLATORS [J].
DAIDO, H .
PROGRESS OF THEORETICAL PHYSICS, 1986, 75 (06) :1460-1463
[10]   POPULATION-DYNAMICS OF RANDOMLY INTERACTING SELF-OSCILLATORS .1. TRACTABLE MODELS WITHOUT FRUSTRATION [J].
DAIDO, H .
PROGRESS OF THEORETICAL PHYSICS, 1987, 77 (03) :622-634