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Optimizing doubly-resonant photonic crystal cavity modes for second harmonic generation

机译:优化双共振光子晶体腔模以产生二次谐波

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We optimize a photonic crystal slab for the generation of second harmonic. The optimization consists in two steps. In the first step a regular photonic crystal, consisting in a triangular lattice of circular holes in a dielectric slab, is optimized by allowing for holes of three alternating radii, with the objective of obtaining a high-frequency bandgap doubly resonant with the fundamental one. The second step consists in modeling a L3 defect cavity in such a photonic crystal where, by further varying the radii and positions of a few neighboring holes, doubly resonant modes at the fundamental and second harmonic frequencies are obtained, with maximal Q-factors and field overlap. The structure emerging from this optimization procedure has Q-factors of 3400 for the fundamental mode and of 430 for the doubly resonant one. Due to the localized nature of those modes and hence their large field overlap, efficient second-harmonic generation is expected in a material with a x~((2)) non-linearity.
机译:我们优化了光子晶体平板,以产生二次谐波。优化包括两个步骤。第一步,通过允许三个交替半径的孔来优化由介电板中的圆形孔的三角形晶格组成的规则光子晶体,以期获得与基频双共振的高频带隙。第二步是在这种光子晶体中对L3缺陷腔进行建模,通过进一步改变一些相邻孔的半径和位置,获得基频和二次谐波频率下的双共振模式,并具有最大的Q因子和场交叠。从该优化过程中出现的结构对于基本模式具有3400的Q因子,对于双共振模式具有430的Q因子。由于这些模式的局部性质,因此它们的大场重叠,在具有x〜((2))非线性的材料中,期望有效的二次谐波产生。

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