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首页> 外文期刊>Journal of Applied Physics >Transmission of terahertz wave through one-dimensional photonic crystals containing single and multiple metallic defects
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Transmission of terahertz wave through one-dimensional photonic crystals containing single and multiple metallic defects

机译:太赫兹波通过包含单个和多个金属缺陷的一维光子晶体的透射

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摘要

We investigated numerically and experimentally the transmission of terahertz (THz) waves through single and multiple metallic defects created in a one-dimensional (ID) photonic crystal (PC) by inserting single metallic wires or arrays of parallel metallic wires into the air-gap defect of the ID PC. The transmission properties of the metallic defect modes generated in the photonic bandgap (PBG) were characterized by using THz time-domain spectroscopy. For single metallic defects, it was found that the appearance the defect mode depends not only on the diameter of the metallic wires but also on the polarization of the THz wave. For transverse magnetic (TM) polarized waves whose electric fields are parallel to the metallic wires, the incident THz wave is generally split into two identical parts. In sharp contrast, the excitation of surface plasmon polaritons (SPPs) with enhanced field intensity is observed for transverse electric (TE) polarized waves whose electric fields are perpendicular to the metallic wires. In both cases, two resonant modes with reduced transmittance are observed in the PBG. While the resonant mode related to SPPs is found at the long-wavelength side of the original defect mode, the resonant mode without the excitation of SPPs appears at the short-wavelength side. Numerical simulation based on the finite-difference time-domain (FDTD) technique revealed that the electric field of SPPs is more tightly confined at the surface of the metallic wire when it is placed in the PC, implying that the confinement of a THz wave in the propagation direction will facilitate the localization of SPPs in the transverse direction. For two parallel metallic wires, the defect mode was found to depend on the separation between them. If they are widely separated, then the excitation of SPPs is similar to that observed in single metallic wires. However, the excitation of dipole-like SPPs does not occur for two closely packed metallic wires because of their large lateral size. It was also revealed that two parallel metallic wires with a small diameter and a narrow separation could be employed to achieve a significant enhancement, as large as 21.6, for the electric field in between them. More interestingly, the enhancement factor becomes larger when the confinement of the electric field in the propagation direction is increased. For an array of four widely separated wires whose lateral dimension is wider than the diameter of the THz beam, only one resonant mode is observed at the long-wavelength side of the original defect mode. The experimental observations are in good agreement with the simulation results based on the FDTD technique. The enhanced concentration of the electric field of SPPs at the surfaces of metallic defects may be useful for focusing and sensing of THz waves.
机译:我们通过将单根金属线或平行金属线阵列插入气隙缺陷中,通过数值和实验研究了太赫兹(THz)波通过一维(ID)光子晶体(PC)中产生的单个和多个金属缺陷的传输ID PC的。利用太赫兹时域光谱技术表征了在光子带隙(PBG)中产生的金属缺陷模式的传输特性。对于单个金属缺陷,发现缺陷模式的外观不仅取决于金属线的直径,还取决于太赫兹波的极化。对于电场平行于金属线的横向磁(TM)极化波,入射的太赫兹波通常分为两个相同的部分。与之形成鲜明对比的是,对于电场垂直于金属线的横向(TE)极化波,观察到了具有增强的场强的表面等离激元极化子(SPPs)的激发。在这两种情况下,PBG中都观察到两个透射率降低的谐振模式。尽管在原始缺陷模式的长波长侧发现了与SPP相关的谐振模式,但在短波长侧出现了无SPP激发的谐振模式。基于有限差分时域(FDTD)技术的数值模拟表明,当金属丝放置在PC中时,SPP的电场更紧密地限制在​​金属丝的表面,这暗示着THz波的限制是传播方向将有利于SPP在横向方向上的定位。对于两条平行的金属线,发现缺陷模式取决于它们之间的间隔。如果将它们分开,则SPP的激发类似于在单根金属线中观察到的激发。然而,由于两根紧密堆积的金属线的横向尺寸较大,因此不会发生偶极状SPP的激发。还揭示出,可以使用两条直径较小且间距狭窄的平行金属线来实现它们之间的电场的显着增强,最大至21.6。更有趣的是,当电场在传播方向上的限制增加时,增强因子变得更大。对于四根宽分离的导线的阵列,其横向尺寸比太赫兹光束的直径宽,在原始缺陷模式的长波侧只能观察到一个谐振模式。实验结果与基于FDTD技术的仿真结果吻合良好。金属缺陷表面上SPP电场的增强集中可能有助于聚焦和感测THz波。

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  • 来源
    《Journal of Applied Physics》 |2011年第7期|p.073101.1-073101.8|共8页
  • 作者单位

    Laboratory of Photonic Information Technology, School of Information and Optoelectronic Science and Engineering, South China Normal University, Guangzhou 510006, People's Republic of China;

    Laboratory of Photonic Information Technology, School of Information and Optoelectronic Science and Engineering, South China Normal University, Guangzhou 510006, People's Republic of China;

    Laboratory of Photonic Information Technology, School of Information and Optoelectronic Science and Engineering, South China Normal University, Guangzhou 510006, People's Republic of China;

    Laboratory of Photonic Information Technology, School of Information and Optoelectronic Science and Engineering, South China Normal University, Guangzhou 510006, People's Republic of China;

    Laboratory of Photonic Information Technology, School of Information and Optoelectronic Science and Engineering, South China Normal University, Guangzhou 510006, People's Republic of China;

    Department of Condensed Matter Physics and Material Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India;

    Department of Computational Mathematics and Cybernetics, M. V. Lomonosov Moscow State University, Moscow 119992, Russia;

    Department of Computational Mathematics and Cybernetics, M. V. Lomonosov Moscow State University, Moscow 119992, Russia;

  • 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);
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