Solitary Wave Emission in a Planar Waveguide with the Adjoining Linear and Nonlinear Thin Film

J. Jeong, C. Kwak, El-Hang Lee
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Abstract

The spatial soliton in Kerr-like nonlinear media has been the subject of extensive research because of its potential application to all-optical switching [1]. In particular, spatial solitary waves in nonlinear waveguides are of cunent interest because of a novel, very interesting optical bistable and switching effect [2,3]. The soliton coupler, suggested by Heartley et al., is one of the most exciting examples to utilize the threshold effect of spatial soliton emission for the sharp switching devices [4]. The majority of theoretical work to date, however, has been restricted to the planar waveguides consisting of the linear thin film bounded by one or two nonlinear semi-infinite media [2,3]. In this work, we consider a planar waveguide consisting of the adjoining linear and nonlinear guiding thin film covered by two linear semi-infinite media, as shown in Fig. 1. The waveguide configuration has distinctive features: (i) due to the confinement of the nonlinearity, the emitted nonlinear wave is generally a solitary wave rather than a soliton and (ii) it can control the emitted power of the solitary wave and the hysteresis of the optical bistability by varying the thickness of the nonlinear thin film.
具有线性和非线性薄膜的平面波导中的孤波发射
类克尔非线性介质中的空间孤子由于其在全光开关[1]中的潜在应用而受到广泛的研究。特别是非线性波导中的空间孤立波,由于一种新颖的、非常有趣的光双稳态和开关效应而引起了人们的极大兴趣[2,3]。由Heartley等人提出的孤子耦合器是利用空间孤子发射阈值效应用于锐利开关器件[4]的最令人兴奋的例子之一。然而,到目前为止,大多数理论工作都局限于由一个或两个非线性半无限介质包围的线性薄膜组成的平面波导[2,3]。在这项工作中,我们考虑了一个平面波导,它由两个线性半无限介质覆盖的相邻线性和非线性导向薄膜组成,如图1所示。该波导结构具有以下特点:(1)由于非线性的限制,所发射的非线性波一般是孤波而不是孤子;(2)可以通过改变非线性薄膜的厚度来控制孤波的发射功率和光双稳性的滞后。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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