2011
DOI: 10.1017/s0308210510001216
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An index theorem for the stability of periodic travelling waves of Korteweg–de Vries type

Abstract: We consider the stability of periodic travelling-wave solutions to a generalized Korteweg-de Vries (gKdV) equation and prove an index theorem relating the number of unstable and potentially unstable eigenvalues to geometric information on the classical mechanics of the travelling-wave ordinary differential equation. We illustrate this result with several examples, including the integrable KdV and modified KdV equations, the L 2 -critical KdV-4 equation that arises in the study of blow-up and the KdV-1 2 equati… Show more

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Cited by 74 publications
(151 citation statements)
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References 27 publications
(57 reference statements)
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“…The proof follows from the Fredholm alternative and may be found in [BH14, Lemma 6]; see [BJK11] in the case of generalized KdV equations. Here we merely hit the main points.…”
Section: Nondegeneracy Of the Linearizationmentioning
confidence: 99%
See 1 more Smart Citation
“…The proof follows from the Fredholm alternative and may be found in [BH14, Lemma 6]; see [BJK11] in the case of generalized KdV equations. Here we merely hit the main points.…”
Section: Nondegeneracy Of the Linearizationmentioning
confidence: 99%
“…Moreover we relate the latter condition with the momentum and the mass as functions of Lagrange multipliers arising in the traveling wave equation, generalizing that in [BSS87], for instance, in the solitary wave setting. In the case of generalized KdV equations, i.e., m(ξ) = ξ 2 in (1.1), the nonlinear stability of a periodic traveling wave to same period perturbations was determined in [Joh09], for instance, through spectral conditions, which were expressed in terms of eigenvalues of the associated monodromy map (or the periodic Evans function); see also [AP07,APBS06,BJK11,DK10,DN11]. Confronted with nonlocal operators, however, spectral problems may be out of reach by Evans function techniques.…”
Section: Introductionmentioning
confidence: 99%
“…Note however that our conditions in (s) are slightly more general than the prescription of ((s1) or (s2)), in that they do not require θ λλ θ µµ − θ 2 λµ = 0. In the special case when κ is constant, Theorem 5 was essentially already known in the case θ λλ θ µµ − θ 2 λµ = 0, and proved in a slightly different manner in [BJK11]. Indeed, orbital stability with respect to co-periodic perturbations is essentially a consequence of [BJK11, Theorem 1], under the assumption…”
Section: So Our Main Assumptions (H0)-(h1)-(h2)-(h3)mentioning
confidence: 98%
“…, is a Sturm-Liouville operator with periodic coefficients, the main argument in the proof of Lemma 2 relies on Sturm's oscillation theorem, as for instance in Lemma 1 in [BJK11], which concerns the case of a constant κ. The detailed proof is postponed to Appendix B.…”
Section: So Our Main Assumptions (H0)-(h1)-(h2)-(h3)mentioning
confidence: 99%
“…That is, given (a 0 , E 0 , c 0 ) ∈ D with c 0 > 0, we assume that the Jacobian {T, M, P } a,E,c is non-zero. While these re-parametrization conditions may seem obscure, the non-vanishing of these Jacobians has been seen to be essential in both the spectral and non-linear stability analysis of periodic gKdV waves in [BrJ,J1,BrJK]. In particular, these Jacobians have been computed in [BrJK] for several power-law nonlinearities and, in the cases considered, has been shown to be generically non-zero.…”
Section: Preliminariesmentioning
confidence: 99%