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Symmetric and asymmetric localized modes in linear lattices with an embedded pair of χ(2)-nonlinear sites

机译:具有嵌入的χ(2)-非线性位点对的线性晶格中的对称和非对称局部模式

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摘要

We construct families of symmetric, antisymmetric, and asymmetric solitary modes in one-dimensionalnbichromatic lattices with the second-harmonic-generating (χ(2)) nonlinearity concentrated at a pair of sitesnplaced at distance l. The lattice can be built as an array of optical waveguides. Solutions are obtained in annimplicit analytical form, which is made explicit in the case of adjacent nonlinear sites, l = 1. The stability isnanalyzed through the computation of eigenvalues for small perturbations and verified by direct simulations. Innthe cascading limit, which corresponds to a large mismatch q, the system becomes tantamount to the recentlynstudied single-component lattice with two embedded sites carrying the cubic nonlinearity. The modes undergonqualitative changes with the variation of q. In particular, at l u0002 2, the symmetry-breaking bifurcation, whichncreates asymmetric states from symmetric ones, is supercritical and subcritical for small and large values of q,nrespectively, while the bifurcation is always supercritical at l = 1. In the experiment, the corresponding changenof the phase transition between the second and first kinds may be implemented by varying the mismatch, via thenwavelength of the input beam. The existence threshold (minimum total power) for the symmetric modes vanishesnexactly at q = 0, which suggests a possibility to create the solitary mode using low-power beams. The stabilitynof solution families also changes with q.
机译:我们构造一维双色格子中的对称,反对称和不对称孤立模式族,二次谐波生成(χ(2))非线性集中在距离l处的一对位置上。晶格可以被构建为光波导的阵列。解可以以非隐式分析形式获得,在相邻的非线性站点l = 1的情况下,可以明确表示。通过对小扰动的特征值进行计算来分析稳定性,并通过直接仿真进行验证。在级联极限(对应于较大的失配q)的情况下,该系统等同于最近研究的带有两个带有立方非线性的嵌入式位点的单分量晶格。模式随q的变化而发生质的变化。特别是,在l u0002 2处,从q的对称状态创建不对称状态的对称破坏分叉分别对于q的大和小值是超临界和亚临界的,而在l = 1时分叉始终是超临界的。第二种和第一种之间的相变的相应改变可以通过输入光束的波长改变失配来实现。对称模式的存在阈值(最小总功率)在q = 0时几乎消失,这表明有可能使用低功率光束创建孤立模式。解族的稳定性也随q改变。

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  • 来源
    《PHYSICAL REVIEW A》 |2012年第1期|1-7|共7页
  • 作者单位

    Centro de F´ısica do Porto Faculdade de Ciˆencias Universidade do Porto R. Campo Alegre 687 4169-007 Porto Portugal;

    Department of Physical Electronics School of Electrical Engineering Faculty of Engineering Tel Aviv University Tel Aviv 69978 Israel;

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