2010
DOI: 10.1016/j.physd.2010.03.005
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Periodic finite-genus solutions of the KdV equation are orbitally stable

Abstract: The stability of periodic solutions of partial differential equations has been an area of increasing interest in the last decade. The KdV equation is known to have large families of periodic solutions that are parameterized by hyperelliptic Riemann surfaces. They are generalizations of the famous multi-soliton solutions. We show that all such periodic solutions are orbitally stable with respect to subharmonic perturbations: perturbations that are periodic with period equal to an integer multiple of the period … Show more

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Cited by 23 publications
(32 citation statements)
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“…The presence of instabilities in shallow water may be surprising, especially in the face of evidence from various asymptotic models such as the Korteweg-de Vries equation (see Bottman &Deconinck 2009 andNivala & and the Benjamin-Bona-Mahoney equation (see Haragus 2008) among others, demonstrating the stability of periodic waves in the context of these asymptotic models describing waves in shallow water. Those equations are all a consequence of long-wave assumptions, and they are not expected to capture the instabilities represented by the bubble eigenvalues.…”
Section: Discussionmentioning
confidence: 99%
“…The presence of instabilities in shallow water may be surprising, especially in the face of evidence from various asymptotic models such as the Korteweg-de Vries equation (see Bottman &Deconinck 2009 andNivala & and the Benjamin-Bona-Mahoney equation (see Haragus 2008) among others, demonstrating the stability of periodic waves in the context of these asymptotic models describing waves in shallow water. Those equations are all a consequence of long-wave assumptions, and they are not expected to capture the instabilities represented by the bubble eigenvalues.…”
Section: Discussionmentioning
confidence: 99%
“…For a fixed µ and a corresponding spectrally stable solution, Ω(ζ) ∈ iR for ζ ∈ R. When ζ ∈ R, the preimage of λ(ζ) ∈ iR is only one point (56) so that by Theorem 1, λ(ζ) is a simple eigenvalue. Therefore, we compute the Krein signature only for ζ ∈ R. From (35),…”
Section: The Advent Of Instabilitymentioning
confidence: 99%
“…When Ω = 0, there exist two bounded eigenfunctions [19,Proposition 3.2]. Only one of these is obtained through (35). We now consider the six values of λ ∈ B.…”
Section: C4 a Proof Of Theoremmentioning
confidence: 99%
“…In exactly the same manner, we further obtain new doubly periodic solutions Finally, from (4) and (12), we get nonlinear rational solution u = 8μ 0 x(12μ 0 t + γ 0 ) (μ 0 x 3 + 12μ 0 t + γ 0 ) 2 .…”
Section: Solutions To the Kdv Equationmentioning
confidence: 99%
“…is a typical soliton equation, it's exact expressions of traveling wave solutions have been studied extensively in many papers [1,2,3,4,5,6]. Especially, the linetwo-soliton solutions obtained by the Inverse scattering method in [7] have been well known.…”
Section: Introductionmentioning
confidence: 99%