利用双色二次间隙孤子的局部化实现全光缓冲

G. Assanto, C. Conti, S. Trillo
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引用次数: 0

摘要

光隙孤子是在非线性波导中实现布拉格谐振光栅全光缓冲和存储器的一种很有前途的方法[1]。事实上,它们允许在实验室框架中定位零速度的电磁能量,在线性传播被禁止的频率范围内。Eggleton等人最近通过Kerr效应在折射率调制光纤中报道了慢传播局域态的实验[2]。然而,在光栅中捕获零速度孤子仍然是一个悬而未决的问题,尽管完全稳定的间隙孤子可以成为全光存储器的基本元素。最近,在参数二次效应的背景下,基于光栅色散、参数增益和级联相移的相互作用,分布反馈光栅(DFBG)结构(布拉格耦合到二次谐波产生(SH G)介质中的一个或两个频率)已被证明支持双色间隙孤子,即困场分量在基频(FF)和二次谐波(SH)处的局域能量态[3-7]。在本文中,我们通过数值证明了平稳间隙模拟可以通过在FF发射的脉冲的非弹性散射在二次非线性DBFG中被激发,并且可以使用类似的“读取”光束被检测到。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
All-optical buffers via localization of two-color quadratic gap solitons
Optical gap solitons are a promising approach towards the realization of all-optical buffers and memories in nonlinear waveguides with Bragg resonant gratings [1]. In fact they permit to localize the e.m. energy at zero-velocity in the laboratory frame, in a frequency range where the linear propagation is otherwise forbidden. A recent experiment on slowly-traveling localized states has been reported by Eggleton et al. in an index-modulated fiber through the Kerr effect [2]. However, the trapping of zero velocity solitons within the grating is still an open issue, despite the fact that perfectly steady gap solitons could become the basic elements in all-optical memories. More recently, in the context of parametric quadratic effects, structures with distributed-feedback gratings (DFBG), Bragg-coupled to one or both frequencies in media for Second-Harmonic Generation (SH G), have been shown to support two-color gap solitons, i.e. localized energy states of trapped field components at the fundamental (FF) and its second harmonic (SH), based on the interplay of grating dispersion, parametric gain and cascading phase shifts [3-7]. In this Communication we numerically demonstrate that stationary gap simultons can be excited in a quadratically nonlinear DBFG via inelastic scattering of pulses launched at the FF, and can be detected using a similar ”reading” beam.
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