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刘强, 赵锦, 孙宇丹, 刘伟, 王建鑫, 刘超, 吕靖薇, 王诗淼, 蒋宇, PaulK.Chu. 365彩票官网官方入口[J]. 365赌球. doi: 10.37188/CO.2022-0025
引用本文: 刘强, 赵锦, 孙宇丹, 刘伟, 王建鑫, 刘超, 吕靖薇, 王诗淼, 蒋宇, PaulK.Chu. 365彩票官网官方入口[J]. 365赌球. doi: 10.37188/CO.2022-0025
LIU Qiang, ZHAO Jin, SUN Yudan, LIU Wei, WANG Jianxin, LIU Chao, LV Jingwei, WANG Shimiao, JIANG Yu, CHU Paul K. 365赌球最新网址[J]. Chinese Optics. doi: 10.37188/CO.2022-0025
Citation: LIU Qiang, ZHAO Jin, SUN Yudan, LIU Wei, WANG Jianxin, LIU Chao, LV Jingwei, WANG Shimiao, JIANG Yu, CHU Paul K. 365赌球最新网址[J]. Chinese Optics. doi: 10.37188/CO.2022-0025

365彩票官网官方入口

  • 1.

    东北石油大学 物理与电子工程学院, 黑龙江 大庆 163318

  • 2.

    大庆师范学院 机电工程学院, 黑龙江 大庆 163712

  • 3.

    香港城市大学 物理系 材料科学与工程系及生物医学工程系, 香港 九龙 999077

详细信息

  • 中图分类号:O433

365赌球最新网址

doi: 10.37188/CO.2022-0025
  • 1.

    School of Physics and Electronic Engineering, Northeast Petroleum University, Daqing 163318, P. R. China

  • 2.

    College of Mechanical and Electrical Engineering, Daqing Normal University, Daqing 163712, P. R. China

  • 3.

    .Department of Physics, Department of Materials Science and Engineering, and Department of Biomedical Engineering, City University of Hong Kong, Tat Chee Avenue, Kowloon, Hong Kong, China

Funds:Supported by the Hainan Province Science and Technology Special Fund (No. ZDYF2022GXJS003); Youth Science Foundation of Northeast Petroleum University (No. 2019QNL-17); Postdoctoral Scientific Research Development Fund of Heilongjiang Province (No. LBH-Q20081);Local Universities Reformation and Development Personnel Training Supporting Project from Central Authorities (No. 140119001), City University of Hong Kong Strategic Research Grant (SRG) (No. 7005505)
More Information
    Author Bio:

    LIU Qiang (1980—), Male, born in Tailai, Heilongjiang, Ph.D, Professor, graduated from Harbin Engineering University in 2012, and is mainly engaged in optical fiber sensing technology. E-mail: [email protected]

    Liu Chao (1978—), Male, born in Mulan, Heilongjiang, Ph.D, Professor, doctoral supervisor, graduated from Harbin Institute of Technology in 2008, and is mainly engaged in micro-structured optical devices. E-mail: [email protected]

    Corresponding author: [email protected]
  • 摘要:

    设计了一种用于甲烷和氢气同时检测的基于表面等离子体共振(SPR)的新型光子准晶体光纤(PQF)传感器。在该传感器中，在银膜上分别沉积Pd-WO3和掺杂聚硅氧烷的笼型分子E薄膜作为氢气和甲烷的敏感材料。采用全矢量有限元方法对PQF-SPR传感器进行了数值分析，证明了该传感器具有良好的传感性能。在0% ~ 3.5%的浓度范围内，氢气的最大检测灵敏度和平均灵敏度分别为0.8 nm/%和0.65 nm/%，甲烷的最大灵敏度和平均灵敏度分别为10 nm/%和8.81 nm/%。该传感器具有同时检测多种气体的能力，在设备小型化和远程监测方面具有很大的潜力。

    Abstract:

    A novel photonic quasi-crystal fiber (PQF) sensor based on surface plasmon resonance (SPR) is designed for simultaneous detection of methane and hydrogen. In the sensor, Pd-WO3 and cryptophane E doped polysiloxane films deposited on silver films are the hydrogen and methane sensing materials, respectively. The PQF-SPR sensor is analyzed numerically by the full-vector finite element method and excellent sensing performance is demonstrated. The maximum and average hydrogen sensitivities are 0.8 nm/% and 0.65 nm/% in the concentration range of 0% to 3.5% and the maximum and average methane sensitivities are 10 nm/% and 8.81 nm/% in the range between 0% and 3.5%. The sensor provides the capability of detecting multiple gases and has large potential in device miniaturization and remote monitoring.

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  • Figure 1. Cross-section of the PQF-SPR sensor.

    Figure 2. Dispersion relationships of the X-polarized core mode and SPP mode, confinement loss spectra, and electric field distributions for C_H 2 = 2.5%: (a) X-polarized core mode at 1875 nm, (b) X-polarized core mode at the phase matching point, and (c) X-polarized SPP mode at 1875 nm.

    Figure 3. Dispersion relationships of the Y-polarized core mode and SPP mode, confinement loss spectra, and electric field distributions for C_CH 4 = 2.5%: (a) Y-polarized core mode at 1570 nm, (b) Y-polarized core mode at the phase matching point, and (c) Y-polarized SPP mode at 1570 nm.

    Figure 4. (a) CL spectra of the core mode for different hydrogen concentrations and (b) CL spectra of the core mode for different methane concentrations .

    Figure 5. Relationship between the gas concentration and wavelength shift for hydrogen and methane.

    Figure 6. (a) CL spectra of the core mode for different air hole diameters d when the hydrogen concentration is 3.0% and (b) Resonance wavelength versus hydrogen concentration (t 1 = t 2 = 30 nm, h 1 = 1.5 μm, h 2 = 2.17 μm, and C_H 2 = 3%).

    Figure 7. (a) CL spectra of the core mode for different air hole diameters d when the methane concentrations are 2.0% and 2.5%; (b) Resonance wavelength versus methane concentration and average sensitivity (t 1 = t 2 = 30 nm, h 1 = 1.5 μm, and h 2 = 2.17 μm).

    Figure 8. (a) CL spectra of the core mode for different metal film thicknesses t 1 at a hydrogen concentration of 3.0% and (b) Resonance wavelength versus hydrogen concentration and average sensitivity (d = 1.58 μm, t 2 = 30 nm, h 1 = 1.5 μm, and h 2 = 2.17 μm)

    Figure 9. (a) CL spectra of the core mode for different metal film thicknesses t 2 when the methane concentrations are 2.0% and 2.5%; (b) Resonance wavelength versus methane concentration and average sensitivity (d = 1.58 μm, t 1 = 30 nm, h 1 = 1.5 μm, and h 2 = 2.17 μm).

    Figure 10. (a) CL spectra of the core mode for different metal film thicknesses h 2 when the methane concentrations are 2.0% and 2.5%; (b) Resonance wavelength versus methane concentration and average sensitivity (d = 1.58 μm, t 1 = t 2 = 30 nm, and h 1 = 1.5 μm).

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365赌球
  • 网络出版日期: 2023-01-13

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