Second-Harmonic Generation from Hyperbolic Plasmonic Nanorod Metamaterial Slab

被引:48
作者
Marino, Giuseppe [1 ,2 ]
Segovia, Paulina [1 ,3 ]
Krasavin, Alexey V. [1 ]
Ginzburg, Pavel [1 ,4 ]
Olivier, Nicolas [1 ,5 ]
Wurtz, Gregory A. [1 ,6 ]
Zayats, Anatoly V. [1 ]
机构
[1] Kings Coll London, Dept Phys, London WC2R 2LS, England
[2] Univ Paris Diderot, CNRS, Mat & Phenomenes Quant, F-75013 Paris, France
[3] CICESE, Dept Opt, Ensenada, Baja California, Mexico
[4] Tel Aviv Univ, Dept Elect Engn, IL-69978 Ramat Aviv, Israel
[5] Univ Sheffield, Dept Phys & Astron, Sheffield S10 2TN, S Yorkshire, England
[6] Univ North Florida, Dept Phys, Jacksonville, FL 32224 USA
基金
英国工程与自然科学研究理事会;
关键词
hyperbolic metamaterials; plasmonics; second harmonic generation; INVERSION SYMMETRY; NANOSTRUCTURES; ENHANCEMENT; MICROSCOPY; REFLECTION; ANTENNA; SURFACE; MEDIA; LIGHT;
D O I
10.1002/lpor.201700189
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
Hyperbolic plasmonic metamaterials provide numerous opportunities for designing unusual linear and nonlinear optical properties. In this work, second-harmonic generation in a hyperbolic metamaterial due to a free-electron nonlinear response of a plasmonic component of the metamaterial is studied. It is shown that owing to a rich modal structure of an anisotropic plasmonic metamaterial slab, the overlap of fundamental and second-harmonic modes results in the broadband enhancement of radiated second-harmonic intensity by up to 2 orders of magnitude for TM- and TE-polarized fundamental light, compared to a smooth Au film under TM-polarised illumination. Compared to the radiated second-harmonic intensity from a bulk LiNbO3 nonlinear crystal of the same thickness, the SHG intensity from a metamaterial slab may be up to 2 orders of magnitude higher at the certain metamaterial resonances. The results open up possibilities to design tuneable frequency-doubling integratable metamaterial with the goal to overcome limitations associated with classical phase matching conditions in thick nonlinear crystals.
引用
收藏
页数:9
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