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Asymptotic stability of the sine-Gordon kink under odd perturbations

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arxiv 2106.09605 v2 pith:RMRHKIAP submitted 2021-06-17 math.AP math-phmath.MP

classification math.APmath-phmath.MP
keywords stabilityasymptotickinksine-gordonperturbationsquadraticklein-gordonlinearized
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abstract

We establish the asymptotic stability of the sine-Gordon kink under odd perturbations that are sufficiently small in a weighted Sobolev norm. Our approach is perturbative and does not rely on the complete integrability of the sine-Gordon model. Key elements of our proof are a specific factorization property of the linearized operator around the sine-Gordon kink, a remarkable non-resonance property exhibited by the quadratic nonlinearity in the Klein-Gordon equation for the perturbation, and a variable coefficient quadratic normal form introduced in [53]. We emphasize that the restriction to odd perturbations does not bypass the effects of the odd threshold resonance of the linearized operator. Our techniques have applications to soliton stability questions for several well-known non-integrable models, for instance, to the asymptotic stability problem for the kink of the $\phi^4$ model as well as to the conditional asymptotic stability problem for the solitons of the focusing quadratic and cubic Klein-Gordon equations in one space dimension.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Classification of kink clusters for scalar fields in dimension 1+1

    math.AP 2024-12 accept novelty 8.0 of 10

    For general 1+1 scalar field models, every kink n-cluster obeys a universal asymptotic law with gaps 2 log(κt) - log(Mk(n-k)/2), and all such clusters form an n-dimensional manifold parameterized by kink positions.

  2. Long time behavior of small solutions of NLS with non-generic potentials in one dimension

    math.AP 2026-07 unverdicted novelty 7.0 of 10

    Small data for 1D cubic NLS with non-generic potentials without symmetry assumptions yield sharp L^∞ decay up to almost-exponential times via a modified distorted Fourier transform.

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