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离散非线性薛定谔系统中的多相自共振激发

Multiphase autoresonant excitations in discrete nonlinear Schrödinger systems.

作者信息

Gopher Y, Friedland L, Shagalov A G

机构信息

Racah Institute of Physics, Hebrew University of Jerusalem, Jerusalem 91904, Israel.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2005 Sep;72(3 Pt 2):036604. doi: 10.1103/PhysRevE.72.036604. Epub 2005 Sep 12.

Abstract

Large amplitude, multiphase solutions of periodic discrete nonlinear Schrödinger (NLS) systems are excited and controlled by starting from zero and using a small perturbation. The approach involves successive formation of phases in the solution by driving the system with small amplitude plane wavelike perturbations (drives) with chirped frequencies, slowly passing through a system's resonant frequency. The system is captured into resonance and enters a continuing phase-locking (autoresonance) stage, if the drive's amplitude surpasses a certain sharp threshold value. This phase-locked solution is efficiently controlled by variation of an external parameter (driving frequency). Numerical examples of excitation of multiphase waves and periodic discrete breathers by using this approach for integrable (Ablowitz-Ladik) and nonintegrable NLS discretizations are presented. The excited multiphase waveforms are analyzed via the spectral theory of the inverse scattering method applied to both the integrable and nonintegrable systems. A theory of autoresonant excitation of 0- and 1-phase solutions by passage through resonances is developed. The threshold phenomenon in these cases is analyzed.

摘要

通过从零点开始并使用小扰动来激发和控制周期性离散非线性薛定谔(NLS)系统的大振幅多相解。该方法包括通过用具有啁啾频率的小振幅平面波状扰动(驱动)驱动系统,使系统的共振频率缓慢通过,从而在解中连续形成相位。如果驱动的振幅超过某个尖锐的阈值,则系统被捕获到共振中并进入持续的锁相(自共振)阶段。通过改变外部参数(驱动频率)可以有效地控制这种锁相解。给出了使用这种方法对可积(阿布洛维茨 - 拉迪克)和不可积NLS离散化激发多相波和周期性离散呼吸子的数值示例。通过应用于可积和不可积系统的逆散射方法的谱理论分析激发的多相波形。发展了通过共振对0相和1相解进行自共振激发的理论。分析了这些情况下的阈值现象。

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