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On The large Time Asymptotics of Schrödinger type equations with General Data

Avy Soffer, Xiaoxu Wu

TL;DR

This work establishes sharp long-time asymptotics for Schrödinger-type equations with general, time-dependent and nonlinear interactions by constructing a novel Free Channel Wave Operator and proving a decomposition of global solutions into a free component plus a weakly localized remainder. The authors develop a phase-space, microlocal framework with propagation and relative-propagation estimates, enabling Cook-like arguments to pass to the limit and to handle both spatially localized and charge-transfer-type interactions in arbitrary dimensions. The results include the existence of adapted wave operators in dimensions n≥3, independence of the localization parameters, and the appearance of moving weakly localized components in the charge-transfer case, with scattering demonstrated in 3D when the nonfree part is small. Overall, the paper extends the Liu–Soffer program to general data and localized interactions, offering a robust toolkit for multichannel scattering and asymptotic completeness in time-dependent settings with potential applications to nonlinear Schrödinger equations with moving potentials.

Abstract

For the Schrödinger equation with a general interaction term, which may be linear or nonlinear, time dependent and including charge transfer potentials, we prove the global solutions are asymptotically given by the sum of a free wave and a weakly localized part. The proof is based on constructing in a new way the Free Channel Wave Operator, and further tools from the recent works \cite{Liu-Sof1,Liu-Sof2,SW2020}. This work generalizes the results of the first part of \cite{Liu-Sof1,Liu-Sof2} to arbitrary dimension, and non-radial data.

On The large Time Asymptotics of Schrödinger type equations with General Data

TL;DR

This work establishes sharp long-time asymptotics for Schrödinger-type equations with general, time-dependent and nonlinear interactions by constructing a novel Free Channel Wave Operator and proving a decomposition of global solutions into a free component plus a weakly localized remainder. The authors develop a phase-space, microlocal framework with propagation and relative-propagation estimates, enabling Cook-like arguments to pass to the limit and to handle both spatially localized and charge-transfer-type interactions in arbitrary dimensions. The results include the existence of adapted wave operators in dimensions n≥3, independence of the localization parameters, and the appearance of moving weakly localized components in the charge-transfer case, with scattering demonstrated in 3D when the nonfree part is small. Overall, the paper extends the Liu–Soffer program to general data and localized interactions, offering a robust toolkit for multichannel scattering and asymptotic completeness in time-dependent settings with potential applications to nonlinear Schrödinger equations with moving potentials.

Abstract

For the Schrödinger equation with a general interaction term, which may be linear or nonlinear, time dependent and including charge transfer potentials, we prove the global solutions are asymptotically given by the sum of a free wave and a weakly localized part. The proof is based on constructing in a new way the Free Channel Wave Operator, and further tools from the recent works \cite{Liu-Sof1,Liu-Sof2,SW2020}. This work generalizes the results of the first part of \cite{Liu-Sof1,Liu-Sof2} to arbitrary dimension, and non-radial data.
Paper Structure (22 sections, 24 theorems, 366 equations)

This paper contains 22 sections, 24 theorems, 366 equations.

Key Result

Theorem 2.4

Assume $\psi(t)$ is the solution to system SE. Let Assumptions asp: global and asp: nonlocal hold. When the space dimension $n\geq3$, for all $\alpha\in(0,1-2/n)$, the adapted free channel wave operator acting on the initial data $\psi(0)$, defined as exists in $L^2_x(\mathbb{R}^n)$. Furthermore, $\Omega_\alpha^*\psi(0)$ is independent on the choice of $\alpha$ in the following sense: for all $\a

Theorems & Definitions (68)

  • Example 2.1
  • proof
  • Example 2.2
  • proof
  • Example 2.3
  • proof
  • Theorem 2.4: $L^p$ potentials
  • Remark 2.5
  • Remark 2.6
  • Remark 2.7
  • ...and 58 more