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Localized state for nonlinear disordered stark model

Shengqing Hu, Yingte Sun

Abstract

In this paper, we consider the following nonlinear disordered Stark model: $${\bf i}\partial_tu_n+δ(u_{n+1}+u_{n-1})+nu_n+v_nu_n+ε|u_n|^{2}u_n=0,\quad n\in\mathbb{Z}.$$ By employing the diagonalization of the associated linear operators and the KAM theory for nonlinear Hamiltonian systems, we establish that for parameters $δ$ and $\varepsilon$ in a reasonable range, and for most realization of random variables $v=\{v_n\}_{n \in \mathbb{Z}}$, there exist time quasi-periodic and spatially localized states that exhibit arbitrary power-law spatial decay.

Localized state for nonlinear disordered stark model

Abstract

In this paper, we consider the following nonlinear disordered Stark model: By employing the diagonalization of the associated linear operators and the KAM theory for nonlinear Hamiltonian systems, we establish that for parameters and in a reasonable range, and for most realization of random variables , there exist time quasi-periodic and spatially localized states that exhibit arbitrary power-law spatial decay.
Paper Structure (17 sections, 23 theorems, 296 equations)

This paper contains 17 sections, 23 theorems, 296 equations.

Key Result

Theorem 1.1

Consider one-dimensional nonlinear disordered stark model eq1.1. Fix $n_k \in \mathbb{Z}, k=1,\cdots, b$ and $d>0$. Let $\mathcal{J}=\{n_k\}^{b}_{k=1} \in \mathbb{Z}$ and $\mathcal{V}=\{v_{\alpha}\}_{\alpha \in \mathcal{J}} \in \mathbb{R}^b$. Then for $0<\delta< \delta_0=O(\frac{1}{b})$, there exits such that if $\mathcal{V} \in \mathcal{O}_\epsilon$, then equation eq1.1 has solution $u(x,t)$ of t

Theorems & Definitions (45)

  • Theorem 1.1
  • Theorem 2.1
  • Definition 2.2
  • Definition 2.3
  • Lemma 2.4
  • proof
  • Lemma 2.5
  • proof
  • Lemma 2.6
  • proof
  • ...and 35 more