Front Solutions for the Ginzburg-Landau Equation

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+ X is a solution o/(4.5') and if c is sufficiently large, then. X = (XS9 Xc) verifies the differential equation. X'S = MCSXS. + RCS(X), X'C = MCCXC. + RCC(X),. (4.8).
Communications IΠ

Commun. Math. Phys. 152, 221-248 (1993)

Mathematical Physics

© Springer-Verlag 1993

Front Solutions for the Ginzburg-Landau Equation J.-P. Eckmann and Th. Gallay Departement de Physique Theorique, Universite de Geneve, CH-1211 Geneva 4, Switzerland Received June 29, 1992

Abstract. We prove the existence of front solutions for the Ginzburg-Landau equation dtu(x, t) = d2xu(x, t) + (1 - \u(x, t)\2)u{x, t), interpolating between two stationary solutions of the form u(x) = ^/l — q2eiqx with different values of q at x = ± oo. Such fronts are shown to exist when at least one of the q is in the Eckhaus-unstable domain.

1. Introduction We consider the Ginzburg-Landau equation (GL) 2

2

dtu(x, t) = d xu(x, t) + (1 - \u(x, t)\ )u(x, t) ,

(1.1)

where u is a complex-valued function of x e R and ί e R + . This equation has time-independent periodic solutions of the form

uq(x) = J\ -