首页> 外文期刊>Journal of the Optical Society of America, B. Optical Physics >Evaluation of the nonlinear response of plasmonic metasurfaces: Miller's rule, nonlinear effective susceptibility method, and full-wave computation
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Evaluation of the nonlinear response of plasmonic metasurfaces: Miller's rule, nonlinear effective susceptibility method, and full-wave computation

机译:等离子超表面的非线性响应评估:米勒法则,非线性有效磁化率方法和全波计算

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摘要

In this article, the second-harmonic generation (SHG) from gold split-ring resonators is investigated using different theoretical methods, namely, Miller's rule, the nonlinear effective susceptibility method, and full-wave computation based on a surface integral equation method. The results confirm that Miller's rule is, in general, not well suited for the description of SHG from plasmonic metasurfaces. On the other hand, the comparison of the nonlinear effective susceptibility method with full-wave computations shows that this method permits us to evaluate second-harmonic (SH) emission patterns from noncentrosymmetric nanoparticles with good accuracy. However, the nonlinear effective susceptibility method fails to reproduce the multipolar nature of the SH emission from centrosymmetric nanoparticles. This shortcoming is attributed to the intrinsic nature of the nonlinear effective susceptibility method, which neglects the exact positions of the nonlinear sources. The numerical implementations of these two methods are also discussed in detail, revealing that the main limitation of the nonlinear effective susceptibility method, aside from the inaccuracy observed in specific cases, is its higher numerical requirements when several emitting directions need to be considered. This limitation stands for most of the numerical methods used for solving Maxwell's equations at the nanoscale. This work provides clear insight into the limitations and advantages of the different methods available for evaluation of SHG from plasmonic metasurfaces. (C) 2015 Optical Society of America
机译:在本文中,使用不同的理论方法,即米勒法则,非线性有效磁化率方法和基于表面积分方程法的全波计算,研究了金裂环谐振器的二次谐波(SHG)。结果证实,米勒法则通常不适合用于描述等离激元超表面的SHG。另一方面,非线性有效磁化率方法与全波计算的比较表明,该方法使我们能够以良好的准确性评估非中心对称纳米粒子的二次谐波(SH)发射模式。但是,非线性有效磁化率方法无法重现中心对称纳米颗粒SH发射的多极性质。该缺点归因于非线性有效磁化率方法的固有性质,该方法忽略了非线性源的确切位置。还详细讨论了这两种方法的数值实现,揭示了非线性有效磁化率方法的主要局限性(除了在特定情况下观察到的不准确性外)是在需要考虑多个发射方向时其较高的数值要求。该限制代表了用于在纳米级求解麦克斯韦方程组的大多数数值方法。这项工作提供了清晰的见解,可用于评估等离子超表面的SHG的不同方法的局限性和优势。 (C)2015年美国眼镜学会

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