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arxiv: nlin/0104067 · v1 · pith:S4VUJWHKnew · submitted 2001-04-27 · 🌊 nlin.PS · cond-mat.dis-nn· cond-mat.soft· cond-mat.stat-mech· nlin.CD· physics.flu-dyn

Composite "zigzag" structures in the 1D complex Ginzburg-Landau equation

classification 🌊 nlin.PS cond-mat.dis-nncond-mat.softcond-mat.stat-mechnlin.CDphysics.flu-dyn
keywords zigzagcglebifurcationstructureszigzagscomplexcompositediagram
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We study the dynamics of the one-dimensional complex Ginzburg Landau equation (CGLE) in the regime where holes and defects organize themselves into composite superstructures which we call zigzags. Extensive numerical simulations of the CGLE reveal a wide range of dynamical zigzag behavior which we summarize in a `phase diagram'. We have performed a numerical linear stability and bifurcation analysis of regular zigzag structures which reveals that traveling zigzags bifurcate from stationary zigzags via a pitchfork bifurcation. This bifurcation changes from supercritical (forward) to subcritical (backward) as a function of the CGLE coefficients, and we show the relevance of this for the `phase diagram'. Our findings indicate that in the zigzag parameter regime of the CGLE, the transition between defect-rich and defect-poor states is governed by bifurcations of the zigzag structures.

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