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Silica High-Mesa Waveguide for Infrared Sensing

机译:用于红外传感的二氧化硅高台面波导

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摘要

High-mesa waveguide is attractive as a certain potion of propagation light profiles out of the waveguide, which can be used for infrared absorption. One of the issues for high-mesa waveguide is its high propagation loss, since high propagation loss consumes light power, which restricts sensing limitation. We tried to fabricate silica high-mesa waveguide for its low propagation loss possibility. The implemented waveguide showed the propagation loss of 0.65dB/cm (@ λ=1550nm, w=2.3μm), which is higher than expected value of lower than 0.1dB/cm. We investigated the reason of the high propagation loss and found that the radiation loss took a large part of the propagation loss. For further improvement, we propose under cladding layer thickness of more than 5μm to suppress the propagation loss.
机译:高阶波导是有吸引力的,因为一定数量的传播光分布在波导之外,可用于红外吸收。高台面波导的问题之一是其高传播损耗,因为高传播损耗消耗光功率,这限制了感测限制。我们试图制造石英高台面波导,因为它具有低传播损耗的可能性。所实现的波导显示出0.65dB / cm的传播损耗(λ= 1550nm,w =2.3μm),高于低于0.1dB / cm的期望值。我们调查了高传播损耗的原因,发现辐射损耗占了传播损耗的很大一部分。为了进一步改善,我们建议覆盖层厚度大于5μm,以抑制传播损耗。

著录项

  • 来源
    《電子情報通信学会技術研究報告》 |2013年第448期|91-94|共4页
  • 作者单位

    Interdisciplinary Graduate School of Engineering Sciences (I-EggS), Kyushu University 6-1,Kasugakoen, Kasuga, Fukuoka 816-8580,Japan;

    Interdisciplinary Graduate School of Engineering Sciences (I-EggS), Kyushu University6-1,Kasugakoen, Kasuga, Fukuoka 816-8580,Japan;

    Interdisciplinary Graduate School of Engineering Sciences (I-EggS), Kyushu University6-1,Kasugakoen, Kasuga, Fukuoka 816-8580,Japan;

    NTT Photonics Laboratories 3-1, Morinosato Wakamiya, Atsugi, Kanagawa 243-0198, Japan;

    NTT Photonics Laboratories 3-1, Morinosato Wakamiya, Atsugi, Kanagawa 243-0198, Japan;

    Interdisciplinary Graduate School of Engineering Sciences (I-EggS), Kyushu University6-1,Kasugakoen, Kasuga, Fukuoka 816-8580,Japan;

  • 收录信息
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Silica; High-mesa; Radiation mode;

    机译:二氧化硅高介面;辐射方式;
  • 入库时间 2022-08-18 00:28:08

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