2003
DOI: 10.1103/physrevlett.90.068301
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Vortex Glass and Vortex Liquid in Oscillatory Media

Abstract: We study the disordered, multi-spiral solutions of two-dimensional homogeneous oscillatory media for parameter values at which the single spiral/vortex solution is fully stable. In the framework of the complex Ginzburg-Landau (CGLE) equation, we show that these states, heretofore believed to be static, actually evolve on ultra-slow timescales. This is achieved via a reduction of the CGLE to the evolution of the sole vortex position and phase coordinates. This true defect-mediated turbulence occurs in two disti… Show more

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Cited by 38 publications
(12 citation statements)
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“…In simulations of the CGL ͑Ref. 31 There the velocity distribution function for the defect motion in the frozen vortex regime of the CGL has been captured quite well with simulations of point defects using their previously established interaction laws. It should be noted, however, that the background field behaves chaotically as well and therefore it contributes to the Lyapunov dimension even in the absence of defects.…”
Section: Introductionmentioning
confidence: 69%
“…In simulations of the CGL ͑Ref. 31 There the velocity distribution function for the defect motion in the frozen vortex regime of the CGL has been captured quite well with simulations of point defects using their previously established interaction laws. It should be noted, however, that the background field behaves chaotically as well and therefore it contributes to the Lyapunov dimension even in the absence of defects.…”
Section: Introductionmentioning
confidence: 69%
“…It appears in several different systems, including biological ones [1][2][3][4]. In the context of fluid dynamics, intermittency can be observed in the transition from a laminar to a turbulent regime, where the stationary flow is interrupted by chaotic bursts occurring at irregular time intervals [5].…”
mentioning
confidence: 99%
“…As the linear coupling J increases further, the condensate falls into the SAB state independently of the initial winding number in each component, and the relative phase is fixed at θ s everywhere. Distinction should be made between defects in the relative phase of the striped states and the shock line defects in frozen states which are solutions of the complex Ginzburg-Landau equation [56,57]. The shock line defects are caused by the phase difference between two nearby vortices [56,57], which are basically singlecomponent phenomena for an open-dissipative system.…”
Section: Pattern Formationmentioning
confidence: 99%