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Finite-time singularity versus global regularity for hyper-viscous Hamilton–Jacobi-like equations

Hamid Bellout et al 2003 Nonlinearity 16 1967-1989   doi: 10.1088/0951-7715/16/6/305  Help

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Hamid Bellout1, Said Benachour2 and Edriss S Titi3,4
1 Department of Mathematical Sciences, Northern Illinois University, DeKalb, IL 60115, USA
2 Institut Elie Cartan, Université Henri Poincaré BP 239, F-54506 Vandoeuvre-lés-Nancy Cedex, France
3 Department of Mathematics, and Department of Mechanical and Aerospace Engineering, University of California, Irvine, CA 92697-3875, USA
E-mail: bellout@math.niu.edu, Said.Benachour@antares.iecn.u-nancy.fr and etiti@math.uci.edu
4 Also at: Department of Computer Science and Applied Mathematics, Weizmann Institute of Science, Rehovot 76100, Israel.

Recommended by P Constantin

Abstract. The global regularity for the two- and three-dimensional Kuramoto–Sivashinsky equations is one of the major open questions in nonlinear analysis. Inspired by this question, we introduce in this paper a family of hyper-viscous Hamilton–Jacobi-like equations parametrized by the exponent in the nonlinear term, p, where in the case of the usual Hamilton–Jacobi nonlinearity, p = 2. Under certain conditions on the exponent p we prove the short-time existence of weak and strong solutions to this family of equations. We also show the uniqueness of strong solutions. Moreover, we prove the blow-up in finite time of certain solutions to this family of equations when the exponent p>2. Furthermore, we discuss the difference in the formation and structure of the singularity between the viscous and hyper-viscous versions of this type of equation.

Mathematics Subject Classification: 35Q53, 35K55

Print publication: Issue 6 (November 2003)
Received 19 September 2002, in final form 18 June 2003
Published 22 August 2003

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