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The non-local Fisher–KPP equation: travelling waves and steady states

Henri Berestycki et al 2009 Nonlinearity 22 2813-2844   doi: 10.1088/0951-7715/22/12/002  Help

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Henri Berestycki1, Grégoire Nadin2, Benoit Perthame3,4 and Lenya Ryzhik5
1 EHESS, CAMS, 54 Boulevard Raspail, F-75006 Paris, France
2 Département de Mathématiques et Applications, École Normale Supérieure, 45 rue d'Ulm, F 75230 Paris cedex 05, France
3 UPMC Univ Paris 06, UMR 7598, Laboratoire Jacques-Louis Lions, F-75005, Paris, France and Institut Universitaire de France
4 CNRS, UMR 7598, Laboratoire Jacques-Louis Lions, F-75005, Paris, France
5 Department of Mathematics, University of Chicago, Chicago, IL 60637, USA
E-mail: hb@ehess.fr, nadin@dma.ens.fr, benoit.perthame@upmc.fr and ryzhik@math.uchicago.edu

Recommended by J-P Eckmann

Abstract. We consider the Fisher–KPP equation with a non-local saturation effect defined through an interaction kernel phi(x) and investigate the possible differences with the standard Fisher–KPP equation. Our first concern is the existence of steady states. We prove that if the Fourier transform \hat\phi(\xi) is positive or if the length σ of the non-local interaction is short enough, then the only steady states are u ≡ 0 and u ≡ 1. Next, we study existence of the travelling waves. We prove that this equation admits travelling wave solutions that connect u = 0 to an unknown positive steady state u(x), for all speeds cc*. The travelling wave connects to the standard state u(x) ≡ 1 under the aforementioned conditions: \hat\phi(\xi)>0 or σ is sufficiently small. However, the wave is not monotonic for σ large.

Mathematics Subject Classification: 35C07, 35Q92

Print publication: Issue 12 (December 2009)
Received 20 March 2009, in final form 27 August 2009
Published 30 October 2009

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