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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(中英文), 2022, 15(1): 101-110. doi: 10.37188/CO.EN.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(中英文), 2022, 15(1): 101-110. doi: 10.37188/CO.EN.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, 2022, 15(1): 101-110. doi: 10.37188/CO.EN.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, 2022, 15(1): 101-110. doi: 10.37188/CO.EN.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

详细信息
  • 中图分类号: O433

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

doi: 10.37188/CO.EN.2021-0006
Funds: Supported by Heilongjiang Provincial talent project (No. ts26180221); Youth Science Foundation of Northeast Petroleum University (No. 2019QNL-17); Natural Science Foundation of Heilongjiang Province (No. E2017010); the City University of Hong Kong Strategic Research Grant (SRG) (No. 7005105, No. 7005265); Scientific Research Fund of Sichuan Province Science and Technology Department (No. 2020YJ0137); Local Universities Reformation and Development Personnel Training Supporting Project from Central Authorities (No. 140119001)
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: nepulq@126.com

    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: msm-liu@126.com

    Corresponding author: msm-liu@126.com
  • 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。该传感器性能优良,在液体折射率测量方面具有很大的应用潜力。

     

  • Figure 1.  Schematic diagram 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 vary from 1.35 to 1.4; (b) the resonance wavelength and the wavelength sensitivity versus the refractive index of the analyte; (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 varying with ITO thickness

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

    Figure 7.  (a), (b) Loss spectra for different air hole spacing and analyte refractive indices of 1.395 and 1.4; (c) peak loss and resonant wavelength for different Λ when 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 the sensor in this paper and those proposed 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-coated1.37~1.401570~198015000 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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出版历程
  • 收稿日期:  2021-07-06
  • 修回日期:  2021-07-20
  • 网络出版日期:  2021-09-10
  • 刊出日期:  2022-01-19

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