Physica D 241 (2012) 125–133 Contents lists available at SciVerse ScienceDirect Physica D journal homepage: www.elsevier.com/locate/physd The Symmetric Regularized-Long-Wave equation: Well-posedness and nonlinear stability Carlos Banquet Brango Departamento de Matemáticas y Estadística, Universidad de Córdoba, Carrera 6 No. 76-103, Montería, Córdoba, Colombia article info Article history: Received 4 May 2011 Received in revised form 17 October 2011 Accepted 19 October 2011 Available online 26 October 2011 Communicated by J. Bronski Keywords: Periodic travelling waves Nonlinear stability Symmetric Regularized Long Wave equation Well-posedness abstract The focus of the present work is the Symmetric Regularized-Long-Wave equation. We prove that the initial value problem for this equation is locally and globally well-posed in H s per × H s1 per and H s (R) × H s1 (R), if s 0. We also prove the existence and nonlinear stability of periodic travelling wave solutions, of cnoidal type, for the equation mentioned above. © 2011 Elsevier B.V. All rights reserved. 1. Introduction In this paper, we study different aspects of the Symmetric Regularized-Long-Wave equation (SRLW equation henceforth) u tt u xx + (uu x ) t u xxtt = 0, (1.1) where u is a real-valued function and the subscripts denote the derivative with respect to the spatial variable x and time t . The Symmetric Regularized-Long-Wave equation is a model for the weakly nonlinear ion acoustic and space-charge waves. This equa- tion was introduced by Seyler and Fenstermacher in [1], where a weakly nonlinear analysis of the cold-electron fluid equation is made. Eq. (1.1) has the equivalent form u t u xxt + uu x v x = 0, v t u x = 0, (1.2) for all t > 0 and x R. This equivalent system has four conserva- tion laws Tel.: +57 3145933379. E-mail addresses: cabanquet@hotmail.com, cbanquet@correo.unicordoba.edu.co. E (u,v) = ∫ uv 1 6 u 3 dx, V (u,v) = 1 2 (u 2 + u 2 x + v 2 )dx, I 1 (u,v) = u dx and I 2 (u,v) = v dx. (1.3) The first aspect that we study about the SRLW equation is the local and global well-posedness. On the periodic case, we prove that Eq. (1.2) with initial data (u 0 ,v 0 ) H s per ([−L, L]) × H s1 per ([−L, L]) is globally well-posed if s 0. The more important ingredient here is a bilinear estimative obtained by Roumégoux in [2]. On the continuous case (this is for initial data in H s (R) × H s1 (R)), we used the ideas given in [3] to prove that (1.2) with initial data (u 0 ,v 0 ) H s (R) × H s1 (R) is globally well-posed if s 0. This result improves the theory established by Chen [4], where a global well-posedness result was proved in H 1 (R) ×L 2 (R). Another important part of this paper is to establish the existence and nonlinear stability of periodic travelling wave solutions for Eq. (1.1). It is well known that the study of this kind of states of motion is very important to understand the behaviour of many physical systems. In the past two decades, various results about nonlinear stability for some equations and systems have been obtained; see for example [5–24]. In this work, we are interested in giving a stability theory of periodic travelling wave solutions for the nonlinear system (1.2). 0167-2789/$ – see front matter © 2011 Elsevier B.V. All rights reserved. doi:10.1016/j.physd.2011.10.007