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Abdon Moutinho

Publications and source records attributed to Abdon Moutinho.

7 recordsLinked to original sources

Asymptotic Stability of multi-solitons for $1$d Supercritical NLS

We consider the one-dimensional $L^2$-supercritical nonlinear Schrödinger equation \[ i\partial_t ψ+ \partial_x^2 ψ+ |ψ|^{2k}ψ= 0, \qquad k>2. \] In this regime solitary waves are spectrally unstable and dispersion is weak. In the pioneering work of Krieger and Schlag~\cite{KriegerSchlag}, asymptotic stability of a single soliton was established on a codimension-one center-stable manifold. We prove asymptotic stability of well-separated multi-solitons on a finite-codimension center-stable manifold. Specifically, for $k>\frac{11}{4}$, perturbations lying on a codimension-$m$ Lipschitz manifold around a superposition of $m$ solitons with distinct velocities converge in $H^1(\mathbb{R})$ to a sum of modulated solitons plus dispersive radiation. Due to the comparatively weak dispersion in one dimension, the analysis of multi-soliton dynamics is considerably more delicate. Existing full-line asymptotic stability results for multi-solitons in non-integrable dispersive equations treat only two solitons and rely on strong relative velocity assumptions together with additional structural conditions on the nonlinearity. Our proof combines a modulation analysis, a refined linear theory for one-dimensional matrix charge transfer models developed in our earlier works~\cite{dispanalysis1,dispanalysis2} together with carefully designed norms that capture the interactions of multiple moving solitons. Our result applies to arbitrarily many solitons with the natural power-type nonlinearity in the $L^2$-supercritical regime under the sole requirements of distinct velocities and sufficient spatial separation.

math.AP

Scattering Theory and dispersive estimates for general $1$d Charge Transfer Models

We continue our study of scattering theory and dispersive properties for one-dimensional charge transfer models, namely linear Schrödinger equations with multiple moving potentials. By the discovery of a refined structure of the construction of distorted Fourier transforms adapted to the multi-potential framework, we remove the large-velocity separation assumption imposed in [8]. This work thus completes the full scattering theory and dispersive analysis for general one-dimensional charge transfer models. These dispersive estimates provide the foundation for analyzing asymptotic stability and collision phenomena for multi-solitons in a general setting.

math.AP

Dispersive analysis for one-dimensional charge transfer models

In this paper, we study one-dimensional linear Schrödinger equations with multiple moving potentials, known as transfer charge models. Focusing on the non-self-adjoint setting that arises in the study of solitons, we systematically develop the scattering theory and establish dispersive estimates under the assumption that the potentials move at significantly different velocities, even in the presence of unstable modes. In particular, we prove the existence of wave operators, asymptotic completeness, and pointwise decay of solutions, without requiring the absence of threshold resonances. Our analysis set up the fundamental work for studying the nonlinear dynamics of multi-solitons, including asymptotic stability and collisions.

math.AP

Collision of two solitons for $1d$ Nonlinear Schrodinger Equation with the same mass

We study the global dynamics of the collision of two solitons having the same mass for one-dimensional Nonlinear Schrödinger models with multi-power nonlinearity. For any natural number k, it is verified that if the incoming speed v between the two solitary waves is small enough, then, after the collision, the two solitons will move away with an outcoming speed v_{f}=v+O(v^{k}) and the remainder of the solution will also have energy and weighted norms of order O(v^{k}). This is applied to the one-dimensional models with polynomial odd nonlinearity having a stable soliton such as the cubic NLS and the cubic-quintic NLS.

math.AP

On the kink-kink collision problem of for the $ϕ^{6}$ model with low speed

We study the elasticity of the collision of two kinks with an incoming low speed $v\in (0,1)$ for the nonlinear wave equation in dimension $1+1$ known as the $ϕ^{6}$ model. We prove for any $k\in\mathbb{N}$ that if the incoming speed $v$ is small enough, then, after the collision, the two kinks will move away with a velocity $v_{f}$ such that $\vert v_{f}-v\vert\leq v^{k}$ and the energy of the remainder will also be smaller than $v^{k}.$ This manuscript is the continuation of our previous paper where we constructed a sequence $ϕ_{k}$ of approximate solutions for the $ϕ^{6}$ model. The proof of our main result relies on the use of the set of approximate solutions from our previous work, modulation analysis, and a refined energy estimate method to evaluate the precision of our approximate solutions during a large time interval.

math.AP

Approximate kink-kink solutions for the $ϕ^{6}$ model in the low-speed limit

This manuscript is the first of a series of two papers that study the problem of elasticity and stability of the collision of two kinks with low speed $v$ for the nonlinear wave equation known as the $ϕ^{6}$ model in dimension $1+1$. In this paper, we construct a sequence of approximate solutions $(ϕ_{k}(v,t,x))_{k\in\mathbb{N}_{\geq 2}}$ for this nonlinear wave equation such that each function $ϕ_{k}(v,t,x)$ converges in the energy norm to the traveling kink-kink with speed $v$ when $t$ goes to $+\infty.$ The methods used in this paper are not restricted only to the $ϕ^{6}$ model.

math.AP

Dynamics of two interacting kinks for the $ϕ^{6}$ model

We consider the nonlinear wave equation known as the $ϕ^{6}$ model in dimension 1+1. We describe the long time behavior of all the solutions of this model close to a sum of two kinks with energy slightly larger than twice the minimum energy of non constant stationary solutions. We prove orbital stability of two moving kinks. We show for low energy excess $ε$ that these solutions can be described for long time less o equivalent than $-\ln{(ε)}ε^{-\frac{1}{2}}$ as the sum of two moving kinks such that each kink's center is close to an explicit function which is a solution of an ordinary differential system. We give an optimal estimate in the energy norm of the remainder $(g(t),\partial_{t}g(t))$ and we prove that this estimate is achieved during a finite instant $t=T\lesssim -\ln{(ε)}ε^{-\frac{1}{2}}.$

math.AP