4.7 Article

Spatially extended dislocations produced by the dispersive Swift-Hohenberg equation

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PHYSICAL REVIEW E
卷 107, 期 4, 页码 -

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AMER PHYSICAL SOC
DOI: 10.1103/PhysRevE.107.044214

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Motivated by previous results, we studied the Swift-Hohenberg equation with an added linear dispersive term, called the dispersive Swift-Hohenberg equation (DSHE). The DSHE produces stripe patterns with spatially extended defects known as seams. These seams correspond to spiral waves in the anisotropic complex Ginzburg-Landau equation (ACGLE) and tend to organize themselves into chains. analytical and numerical results confirm these findings.
Motivated by previous results showing that the addition of a linear dispersive term to the two-dimensional Kuramoto-Sivashinsky equation has a dramatic effect on the pattern formation, we study the Swift-Hohenberg equation with an added linear dispersive term, the dispersive Swift-Hohenberg equation (DSHE). The DSHE produces stripe patterns with spatially extended defects that we call seams. A seam is defined to be a dislocation that is smeared out along a line segment that is obliquely oriented relative to an axis of reflectional symmetry. In contrast to the dispersive Kuramoto-Sivashinsky equation, the DSHE has a narrow band of unstable wavelengths close to an instability threshold. This allows for analytical progress to be made. We show that the amplitude equation for the DSHE close to threshold is a special case of the anisotropic complex Ginzburg-Landau equation (ACGLE) and that seams in the DSHE correspond to spiral waves in the ACGLE. Seam defects and the corresponding spiral waves tend to organize themselves into chains, and we obtain formulas for the velocity of the spiral wave cores and for the spacing between them. In the limit of strong dispersion, a perturbative analysis yields a relationship between the amplitude and wavelength of a stripe pattern and its propagation velocity. Numerical integrations of the ACGLE and the DSHE confirm these analytical results.

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