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Discrete nonlinear wave propagation in Kerr nonlinear media.

机译:离散非线性波在Kerr非线性介质中的传播。

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摘要

Discrete optical systems are a subgroup of periodic structures in which the evolution of a continuous electromagnetic field can be described by a discrete model. In this model, the total field is the sum of localized, discrete modes. Weakly coupled arrays of single mode channel waveguides have been known to fall into this class of systems since the late 1960's. Nonlinear discrete optics has received a considerable amount of interest in the last few years, triggered by the experimental realization of discrete solitons in a Kerr nonlinear AlGaAs waveguide array by H. Eisenberg and coworkers in 1998.; In this work a detailed experimental investigation of discrete nonlinear wave propagation and the interactions between beams, including discrete solitons, in discrete systems is reported for the case of a strong Kerr nonlinearity.; The possibility to completely overcome "discrete" diffraction and create highly localized solitons, in a scalar or vector geometry, as well as the limiting factors in the formation of such nonlinear waves is discussed. The reversal of the sign of diffraction over a range of propagation angles leads to the stability of plane waves in a material with positive nonlinearity. This behavior can not be found in continuous self-focusing materials where plane waves are unstable against perturbations. The stability of plane waves in the anomalous diffraction region, even at highest powers, has been experimentally verified.; The interaction of high power beams and discrete solitons in arrays has been studied in detail. Of particular interest is the experimental verification of a theoretically predicted unique, all optical switching scheme, based on the interaction of a so called "blocker" soliton with a second beam. This switching method has been experimentally realized for both the coherent and incoherent case. Limitations of such schemes due to nonlinear losses at the required high powers are shown.
机译:离散光学系统是周期性结构的子集,其中可以通过离散模型描述连续电磁场的演变。在此模型中,总场是局部离散模式之和。自1960年代末以来,单模通道波导的弱耦合阵列已属于此类系统。 H. Eisenberg及其同事在1998年通过在Kerr非线性AlGaAs波导阵列中实现离散孤子的实验触发了非线性离散光学的巨大兴趣。在这项工作中,针对强Kerr非线性的情况,报告了在离散系统中离散非线性波传播以及包括离散孤子在内的光束之间相互作用的详细实验研究。讨论了在标量或矢量几何中完全克服“离散”衍射并产生高度局部孤子的可能性,以及形成此类非线性波的限制因素。在一定传播角范围内,衍射符号的反转导致具有正非线性的材料中平面波的稳定性。这种现象在平面波对扰动不稳定的连续自聚焦材料中找不到。实验证明,即使在最高功率下,平面波在异常衍射区域的稳定性也是如此。已经对高功率光束与离散孤子在阵列中的相互作用进行了详细研究。特别令人感兴趣的是,基于所谓的“阻挡”孤子与第二束光束的相互作用,对理论上预测的独特的全光切换方案进行实验验证。对于相干和不相干的情况,已经通过实验实现了这种切换方法。示出了由于所需的高功率下的非线性损耗而导致的这种方案的局限性。

著录项

  • 作者

    Meier, Joachim.;

  • 作者单位

    University of Central Florida.;

  • 授予单位 University of Central Florida.;
  • 学科 Physics Optics.
  • 学位 Ph.D.
  • 年度 2004
  • 页码 136 p.
  • 总页数 136
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 光学;
  • 关键词

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