Adiabatic mode coupler on ion-exchanged waveguides for the efficient excitation of surface plasmon modes (Presentation Recording)

Josslyn Beltran Madrigal, M. Berthel, F. Gardillou, Ricardo Tellez Limon, C. Couteau, D. Barbier, A. Drezet, R. Salas-Montiel, S. Huant, S. Blaize, W. Geng
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Abstract

Several works have already shown that the excitation of plasmonic structures through waveguides enables a strong light confinement and low propagation losses [1]. This kind of excitation is currently exploited in areas such as biosensing [2], nanocircuits[3] and spectroscopy[4]. The efficient excitation of surface plasmon modes (SPP) with guided modes supported by high-index-contrast waveguides, such as silicon-on-insulator waveguides, had already been shown [1,5]. However, the use of weakconfined guided modes of a glass ion exchanged waveguide as a SPP excitation source represents a technological challenge, because the mismatch between the size of their respective electromagnetic modes is so high that the resultant coupling loss is unacceptable for practical applications. In this work, we describe how an adiabatic taper structure formed by an intermediate high-index-contrast layer placed between a plasmonic structure and an ion-exchanged waveguide decreases the mismatch between effective indices, size, and shape of the guided modes. This hybrid structure concentrates the electromagnetic energy from the micrometer to the nanometer scale with low coupling losses to radiative modes. The electromagnetic mode confined to the high-index-contrast waveguide then works as an efficient source of SPP supported by metallic nanostructures placed on its surface. We theoretically studied the modal properties and field distribution along the adiabatic coupler structure. In addition, we fabricated a high-index-contrast waveguide by electron beam lithography and thermal evaporation on top of an ion-exchanged waveguide on glass. This structure was characterized with the use of near field scanning optical microscopy (NSOM). Numerical simulations were compared with the experimental results. [1] N. Djaker, R. Hostein, E. Devaux, T. W. Ebbesen, and H. Rigneault, and J. Wenger, J. Phys. Chem. C 114, 16250 (2010). [2] P. Debackere, S. Scheerlinck, P. Bienstman, R. Baets, Opt. Express 14, 7063 (2006).] [3] A. A. Reiserer, J.-S. Huang, B. Hecht, and T. Brixner. Opt. Express 18(11), 11810–11820 (2010). [4] R. Salas-Montiel, A. Apuzzo, C. Delacour, Z. Sedaghat, A. Bruyant et al. Appl. Phys Lett 100, 231109 (2012) [5] A. Apuzzo M. Fevier, M. Salas-Montiel et al. Nano letters, 13, 1000-1006
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离子交换波导上用于有效激发表面等离子体模式的绝热模式耦合器(演讲记录)
一些工作已经表明,通过波导激发等离子体结构可以实现强光约束和低传播损耗[1]。这种激发目前被应用于生物传感[2]、纳米电路[3]和光谱学[4]等领域。高折射率对比波导(如绝缘体上硅波导)支持的引导模式有效激发表面等离子体模式(SPP)已经被证明[1,5]。然而,使用玻璃离子交换波导的弱约束引导模式作为SPP激发源是一项技术挑战,因为它们各自的电磁模式尺寸之间的不匹配是如此之高,以至于导致的耦合损失在实际应用中是不可接受的。在这项工作中,我们描述了由放置在等离子体结构和离子交换波导之间的中间高折射率对比层形成的绝热锥度结构如何减少导模的有效折射率、尺寸和形状之间的不匹配。这种混合结构将电磁能量从微米级集中到纳米级,具有低耦合损耗的辐射模式。电磁模式限制在高折射率对比波导中,然后作为放置在其表面的金属纳米结构支撑的SPP的有效来源。从理论上研究了绝热耦合器结构的模态特性和场分布。此外,我们还利用电子束光刻和热蒸发技术在玻璃上的离子交换波导上制作了高折射率对比波导。利用近场扫描光学显微镜(NSOM)对该结构进行了表征。数值模拟结果与实验结果进行了比较。[1]李建军,李建军,李建军,等。化学。[j] .农业科学,2010(5)。[2]张建军,张建军,张建军,等。中国生物医学工程学报,2014,33(2):481 - 481。[3]李志强,李志强。黄,B. Hecht和T. Brixner。光学学报,18(11),1181 - 1181(2010)。[4]张晓明,张晓明,张晓明,等。达成。[5]张晓明,张晓明,张晓明,等。生物多样性研究进展与展望[j] .中国生物医学工程学报,2014,32(5):559 - 567。纳米字母,13,1000 -1006
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