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Numerical investigation of optical Tamm states in two-dimensional hybrid plasmonic-photonic crystal nanobeams

机译:二维等离激元-光子晶体纳米束中光学Tamm态的数值研究

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摘要

Optical Tamm states (OTSs) in analogy with its electronic counterpart confined at the surface of crystals are optical surface modes at the interfaces between uniform metallic films and distributed Bragg reflectors. In this paper, OTSs are numerically investigated in two-dimensional hybrid plasmonic-photonic crystal nanobeams (HPPCN), which are constructed by inserting a metallic nanoparticle into a photonic crystal nanobeam formed by periodically etching square air holes into dielectric waveguides. The evidences of OTSs can be verified by transmission spectra and the field distribution at resonant frequency. Similar to OTSs in one-dimensional multilayer structures OTSs in HPPCN can be excited by both TE and TM polarization. The physical origin of OTSs in HPPCN is due to the combined contribution of strong reflection imposed by the photonic band gap (PBG) of the photonic crystal (PC) nanobeam and strong backward scattering exerted by the nanoparticle. For TE, incidence OTSs can be obtained at the frequency near the center of the photonic band gap. The transmissivity and the resonant frequency can be finely tuned by the dimension of nanopar-ticles. While for TM incidence OTSs are observed for relatively larger metallic nanoparticles compared with TE polarization. The differences between TE and TM polarization can be explained by two reasons. For one reason stronger backward scattering of nanoparticles for TE polarization can be achieved by the excitation of localized surface plasmon polariton of nanoparticles. This assumption has been proved by examining the scattering, absorption, and extinction cross section of the metallic nanoparticle. The other can be attributed to the deep and wide PBG available for TE polarization with less number of air holes compared with TM polarization. Our results show great promise in extending the application scope of OTSs from one-dimensional structures to practical integrated photonic devices and circuits.
机译:光学塔姆态(OTSs)与限制在晶体表面的电子对应物类似,是在均匀金属膜和分布式布拉格反射器之间的界面处的光学表面模式。在本文中,在二维混合等离子-光子晶体纳米束(HPPCN)中对OTS进行了数值研究,其是通过将金属纳米粒子插入通过周期性刻蚀介电波导中的方形气孔而形成的光子晶体纳米束中而构建的。 OTS的证据可以通过透射光谱和共振频率下的场分布来验证。类似于一维多层结构中的OTS,HPPCN中的OTS可以通过TE和TM极化激发。 HPPCN中OTS的物理起源是由于光子晶体(PC)纳米束的光子带隙(PBG)施加的强反射和纳米粒子施加的强向后散射的共同作用。对于TE,可以在光子带隙中心附近的频率处获得入射OTS。透射率和共振频率可以通过纳米粒子的尺寸进行微调。对于TM入射,与TE极化相比,在相对较大的金属纳米颗粒中观察到了OTS。 TE和TM极化之间的差异可以通过两个原因来解释。出于一个原因,可以通过激发纳米粒子的局部表面等离子体激元极化来实现纳米粒子对TE极化的更强的向后散射。通过检查金属纳米粒子的散射,吸收和消光截面已证明了这一假设。另一个可以归因于可用于TE极化的深而宽的PBG,与TM极化相比,气孔数量更少。我们的结果显示了将OTS的应用范围从一维结构扩展到实际集成光子器件和电路的巨大希望。

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  • 来源
    《Journal of Applied Physics》 |2014年第4期|043106.1-043106.7|共7页
  • 作者单位

    School of Physics and Optoelectronic Engineering, Guangdong University of Technology, Guangzhou 510006, People's Republic of China;

    School of Physics and Optoelectronic Engineering, Guangdong University of Technology, Guangzhou 510006, People's Republic of China;

    School of Physics and Optoelectronic Engineering, Guangdong University of Technology, Guangzhou 510006, People's Republic of China;

    Laboratory of Optical Physics, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China;

    Laboratory of Optical Physics, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China;

    Laboratory of Optical Physics, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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