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Scattering and localized states for defocusing nonlinear Schrödinger equations with potential

Avy Soffer, Gavin Stewart

TL;DR

The article develops a robust framework to understand the long-time behavior of 1D defocusing NLS with a localized potential by combining exterior Morawetz and exterior interaction Morawetz estimates with an incoming/outgoing decomposition. It proves that global H^1 solutions split into a free radiation part and a weakly localized remainder, with mass concentrating at |x| ≤ t^{1/2+} and energy at |x| ≤ t^{1/3+}; these results hold for arbitrarily large initial data. In the mass-supercritical regime, it constructs a free-channel wave operator in H^1, establishing a precise asymptotic channel behavior and slow spreading for the remainder. The work advances the soliton-resolution program in time-dependent, nontrivial potentials by providing quantitative exterior-space control that compensates for the lack of strong dispersion in one dimension.

Abstract

We study the large-time behavior of global energy class ($H^1$) solutions of the one-dimensional nonlinear Schrödinger equation with a general localized potential term and a defocusing nonlinear term. By using a new type of interaction Morawetz estimate localized to an exterior region, we prove that these solutions decompose into a free wave and a weakly localized part which is asymptotically orthogonal to any fixed free wave. We further show that the $L^2$ norm of this weakly localized part is concentrated in the region $|x| \leq t^{1/2+}$, and that the energy ($\dot{H}^1$) norm is concentrated in $|x| \leq t^{1/3+}$. Our results hold for solutions with arbitrarily large initial data.

Scattering and localized states for defocusing nonlinear Schrödinger equations with potential

TL;DR

The article develops a robust framework to understand the long-time behavior of 1D defocusing NLS with a localized potential by combining exterior Morawetz and exterior interaction Morawetz estimates with an incoming/outgoing decomposition. It proves that global H^1 solutions split into a free radiation part and a weakly localized remainder, with mass concentrating at |x| ≤ t^{1/2+} and energy at |x| ≤ t^{1/3+}; these results hold for arbitrarily large initial data. In the mass-supercritical regime, it constructs a free-channel wave operator in H^1, establishing a precise asymptotic channel behavior and slow spreading for the remainder. The work advances the soliton-resolution program in time-dependent, nontrivial potentials by providing quantitative exterior-space control that compensates for the lack of strong dispersion in one dimension.

Abstract

We study the large-time behavior of global energy class () solutions of the one-dimensional nonlinear Schrödinger equation with a general localized potential term and a defocusing nonlinear term. By using a new type of interaction Morawetz estimate localized to an exterior region, we prove that these solutions decompose into a free wave and a weakly localized part which is asymptotically orthogonal to any fixed free wave. We further show that the norm of this weakly localized part is concentrated in the region , and that the energy () norm is concentrated in . Our results hold for solutions with arbitrarily large initial data.
Paper Structure (36 sections, 20 theorems, 264 equations)

This paper contains 36 sections, 20 theorems, 264 equations.

Key Result

Theorem 1

Suppose $\sigma \geq 2$, that $u$ is a bounded energy solution to eqn:NLS with $p > 1$ and is nonradiative in the sense that there exists $\beta \in (1/3,1)$ such that eqn:nonrad-hypo holds. If $|x|^{1/2}u_0 \in L^2$, then $\langle |x| \rangle_t \lesssim 1 + t^{1/2}$. Furthermore, if $p < { 5}$, the

Theorems & Definitions (41)

  • Theorem 1
  • Remark 1
  • Remark 2
  • Theorem 2
  • Remark 3
  • Remark 4
  • Remark 5
  • Lemma 3
  • proof
  • Theorem 4
  • ...and 31 more