Montagne, R.; Amengual, A.; Hernández-García, E.; San Miguel, M.
Physical Review E 50, 377-385 (1994)
The dynamics of transient patterns formed by front propagation in extended nonequilibrium systems is considered. Under certain circumstances, the state left behind a front propagating into an unstable homogeneous state can be an unstable periodic pattern. It is found by a numerical solution of a model of the Fréedericksz transition in nematic liquid crystals that the mechanism of decay of such periodic unstable states is the propagation of a second front which replaces the unstable pattern by another unstable periodic state with a larger wavelength. The speed of this second front and the periodicity of the new state are analytically calculated with a generalization of the marginal stability formalism suited to the study of front propagation into periodic unstable states.
Link to the paper at Los Alamos preprint server (now arXiv): http://arxiv.org/abs/patt-sol/9312001
DOI | 10.1103/PhysRevE.50.377 |
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ArXiv Number | patt-sol/9312001 |
Files | montagne.ps (1946469 Bytes) montagne.pdf (3938799 Bytes) |
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