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High-sensitivity surface plasmon resonance sensor based on the ten-fold eccentric core quasi-D-shaped photonic quasi-crystal fiber coated with indium tin oxide

LIU Qiang JIANG Yu HU Chun-jie LU Wen-shu SUN Yu-dan LIU Chao LV Jing-wei ZHAO Jin TAI Sheng-nan YI Zao CHU Paul K

刘强, 蒋宇, 胡春杰, 卢文姝, 孙宇丹, 刘超, 吕靖薇, 赵锦, 邰胜男, 易早, PaulK Chu. 基于氧化铟锡的十重偏芯D型光子准晶光纤的高灵敏度表面等离子体共振传感器[J]. 中国光学. doi: 10.37188/CO.2021-0006
引用本文: 刘强, 蒋宇, 胡春杰, 卢文姝, 孙宇丹, 刘超, 吕靖薇, 赵锦, 邰胜男, 易早, PaulK Chu. 基于氧化铟锡的十重偏芯D型光子准晶光纤的高灵敏度表面等离子体共振传感器[J]. 中国光学. doi: 10.37188/CO.2021-0006
LIU Qiang, JIANG Yu, HU Chun-jie, LU Wen-shu, SUN Yu-dan, LIU Chao, LV Jing-wei, ZHAO Jin, TAI Sheng-nan, YI Zao, CHU Paul K. High-sensitivity surface plasmon resonance sensor based on the ten-fold eccentric core quasi-D-shaped photonic quasi-crystal fiber coated with indium tin oxide[J]. Chinese Optics. doi: 10.37188/CO.2021-0006
Citation: LIU Qiang, JIANG Yu, HU Chun-jie, LU Wen-shu, SUN Yu-dan, LIU Chao, LV Jing-wei, ZHAO Jin, TAI Sheng-nan, YI Zao, CHU Paul K. High-sensitivity surface plasmon resonance sensor based on the ten-fold eccentric core quasi-D-shaped photonic quasi-crystal fiber coated with indium tin oxide[J]. Chinese Optics. doi: 10.37188/CO.2021-0006

基于氧化铟锡的十重偏芯D型光子准晶光纤的高灵敏度表面等离子体共振传感器

doi: 10.37188/CO.2021-0006

High-sensitivity surface plasmon resonance sensor based on the ten-fold eccentric core quasi-D-shaped photonic quasi-crystal fiber coated with indium tin oxide

Funds: Provincial talent project [ts26180221], Youth Science Foundation of Northeast Petroleum University [15071120517], Natural Science Foundation of Heilongjiang Province [E2017010], the City University of Hong Kong Strategic Research Grant (SRG) [7005105 and 7005265], Scientific Research Fund of Sichuan Province Science and Technology Department [2020YJ0137] and Local Universities Reformation and Development Personnel Training Supporting Project from Central Authorities [140119001]
More Information
    Author Bio:

    刘 强(1980—),男,黑龙江泰来人,博士,教授,2012年毕业于哈尔滨工程大学获得博士学位,主要从事光纤传感技术研究。E-mail:nepulq@126.com

    刘 超(1978—),男,黑龙江木兰人,博士,教授,博士生导师,2008年毕业于哈尔滨工业大学获得博士学位,主要从事微结构光学器件研究。E-mail:msm-liu@126.com

    Corresponding author: msm-liu@126.com (C. Liu)
  • 摘要: 设计并分析了一种高灵敏度表面等离子体共振(SPR)传感器,该传感器由偏芯D型结构的十重光子准晶光纤(PQF)组成,并局部涂覆氧化铟锡(ITO)。偏芯D型结构可以使液体分析更加方便,增强了纤芯模与SPP模之间的耦合,提高了传感灵敏度。采用了有限元法对传感器的特性进行研究,结果表明传感器的波长灵敏度随折射率(RIs)的增大而增大,最大波长灵敏度和分辨率分别为60000 nm/RIU和1.67×10?6 RIU。该传感器具有优良的性能,在液体折射率测量方面具有很大的应用潜力。
  • Figure  1.  Cross-section of PQF-SPR sensor.

    Figure  2.  Loss spectra of the core modes and dispersion relation between the Y-polarized core mode and SPP mode for a liquid analyte RI of 1.39.

    Figure  3.  Mode field diagrams for the analyte RI of 1.39: (a) Y-polarized core mode and (b) Y-polarized SPP mode.

    Figure  4.  (a) Loss spectra as the analyte RIs are varied from 1.35 to 1.4; (b) The resonance wavelength versus refractive index of the analyte and the wavelength sensitivity; (c) Amplitude sensitivity curves of the sensor for analyte RIs between 1.35 and 1.395.

    Figure  5.  (a) Loss spectra of the samples with different ITO thicknesses and (b) Wavelength sensitivity versus ITO thickness.

    Figure  6.  (a) Loss spectra for different ITO lengths for refractive indexes of 1.395 and 1.4 and (b) Variation of the resonance wavelength with ITO lengths.

    Figure  7.  (a) and (b) Loss spectra for different air hole space and analyte refractive indexes of 1.395 and 1.4; (c) Peak loss and resonant wavelength for different Λ for na=1.395 and na=1.4.

    Figure  8.  (a) Loss spectra for different air hole diameters d1 as na = 1.4, (b) Loss spectra for d1 = 2.4 μm and 2.6 μm, (c)The effect of d2 on the loss spectra for na=1.395 and 1.4.

    Table  1.   Sensing performance of the sensor for different analyte RIs.

    Analyte RIPeak wavelength
    (nm)
    Res. Peak Shift
    (nm)
    Wavelength Sensitivity
    (nm/RIU)
    Amp. Sens.
    (RIU?1)
    Wavelength
    Resolution (RIU)
    Amplitude
    Resolution (RIU)
    1.351760306000102.4241.67×10?59.76×10?5
    1.3551790306000110.8341.37×10?59.02×10?5
    1.361820408000127.3851.25×10?57.85×10?5
    1.36518605010000143.6031.00×10?56.96×10?5
    1.3719105010000168.5441.00×10?55.93×10?5
    1.37519606012000200.1918.33×10?65.41×10?5
    1.3820208016000248.5016.25×10?64.02×10?5
    1.385210010020000329.5735.00×10?63.03×10?5
    1.39220015030000516.3433.33×10?61.93×10?5
    1.395235030060000594.2411.67×10?61.68×10?5
    1.42650N/AN/AN/AN/AN/A
    下载: 导出CSV

    Table  2.   Comparison of the performance of our sensor with those in the recent literatures.

    Refs.StructureRI RangeOperation Wave. Range (nm)Wave. Res. (RIU)Max. Wave. Sens. (nm/RIU)
    [19]D-shaped ITO-coated PQF1.26~1.381380~22602.86×10?6 RIU35000 nm/RIU
    [21]D-shaped ITO-coated PCF1.22~1.331200~22506.67×10?6 RIU15000 nm/RIU
    [39]Double groove with Ag and Au1.22~1.361470~21548.68×10?6 RIU12400 nm/RIU
    [34]eccentric core ITO-coated PQF1.33~1.391480~20084.739×10?6 RIU21000 nm/RIU
    [42]Dual core ITO, graphene-coated1.37~1.401570~1980?15000 nm/RIU
    [41]Arc groove PCF-SPR1.22~1.371650~27301.96×10?6 RIU51000 nm/RIU
    [40]Graphene D-shaped PCF-SPR1.33~1.381880~21409.35×10?6 RIU10694 nm/RIU
    This workD-shaped eccentric core PQF1.35~1.401760~26501.67×10?6 RIU60000 nm/RIU
    下载: 导出CSV
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