Example of a chaotic crystal: The labyrinth

M. Le Berre, E. Ressayre, A. Tallet, Y. Pomeau, and L. Di Menza
Phys. Rev. E 66, 026203 – Published 9 August 2002
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Abstract

Labyrinthine structures often appear as the final steady state of pattern forming systems. Being disordered, they exhibit the same kind of short range positional order as the Newell-Pomeau turbulent crystal. Labyrinths can be seen as a limit case of the texture of disordered rolls with a coherence length of the same order as the wavelength. In the various two-dimensional model equations we looked at, labyrinths and parallel rolls are steady states for the same parameters, their occurrence depending on the initial conditions. Comparing the stability of these two structures, we find that in variational models their energy is very close, rolls always being more stable than labyrinths. For the nonvariational model we propose a numerical experiment which displays a well defined bifurcation from parallel rolls to labyrinths as the more stable state.

  • Received 18 December 2001

DOI:https://doi.org/10.1103/PhysRevE.66.026203

©2002 American Physical Society

Authors & Affiliations

M. Le Berre, E. Ressayre, and A. Tallet

  • Laboratoire de Photophysique Moléculaire, Bâtiment 210, Université de Paris–Sud, 91405 Orsay Cedex, France

Y. Pomeau

  • Laboratoire de Physique Statistique de l’ENS, 24 rue Lhomond, 75005 Paris Cedex 05, France

L. Di Menza

  • Laboratoire d’Analyse Numérique et EDP, Bâtiment 425, Université de Paris–Sud, 91405 Orsay Cedex, France

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Vol. 66, Iss. 2 — August 2002

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