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Phys. Rev. E 78, 046201 (2008) [16 pages]

Eckhaus instability and homoclinic snaking

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A. Bergeon
IMFT UMR CNRS 5502–UPS UFR MIG, 31062 Toulouse Cedex, France

J. Burke
Boston University, Center for BioDynamics, 111 Cummington Street, Boston, Massachusetts 02215, USA

E. Knobloch
Department of Physics, University of California, Berkeley, California 94720, USA

I. Mercader
Departament de Física Aplicada, Universitat Politècnica de Catalunya, Barcelona, Spain

Received 23 June 2008; published 1 October 2008

Homoclinic snaking is a term used to describe the back and forth oscillation of a branch of time-independent spatially localized states in a bistable, spatially reversible system as the localized structure grows in length by repeatedly adding rolls on either side. This behavior is simplest to understand within the subcritical Swift-Hohenberg equation, but is also present in the subcritical regime of doubly diffusive convection driven by horizontal gradients. In systems that are unbounded in one spatial direction homoclinic snaking continues indefinitely as the localized structure grows to resemble a spatially periodic state of infinite extent. In finite domains or in periodic domains with finite spatial period the process must terminate. In this paper we show that the snaking branches in general turn over once the length of the localized state becomes comparable to the domain, and examine the factors that determine the location of the termination point or points, and their relation to the Eckhaus instability of the spatially periodic state.

© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevE.78.046201
DOI:
10.1103/PhysRevE.78.046201
PACS:
47.54.−r, 47.20.Ky, 44.25.+f