• Acta Optica Sinica
  • Vol. 41, Issue 19, 1928003 (2021)
Zongren Li1, Hu Deng1、2、3、*, Jieping Yang1, Quancheng Liu1, Jin Guo1, and Liping Shang1、2、3
Author Affiliations
  • 1School of Information Engineering, Southwest University of Science and Technology, Mianyang, Sichuan 621010, China
  • 2Key Laboratory of Special Environment Robotics of Sichuan Province, Mianyang, Sichuan 621010, China
  • 3Joint Laboratory for Extreme Conditions Matter Properties, Research Center of Laser Fusion, China Academy of Engineering Physics, Southwest University of Science and Technology, Mianyang, Sichuan 621010, China
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    DOI: 10.3788/AOS202141.1928003 Cite this Article Set citation alerts
    Zongren Li, Hu Deng, Jieping Yang, Quancheng Liu, Jin Guo, Liping Shang. High-Sensitivity Terahertz Microfluidic Sensor Based on Irregular U-type Structure[J]. Acta Optica Sinica, 2021, 41(19): 1928003 Copy Citation Text show less
    Terahertz microfluidic sensor. (a) Sensor structure; (b) unit metal structure
    Fig. 1. Terahertz microfluidic sensor. (a) Sensor structure; (b) unit metal structure
    Equivalent circuit. (a) LC resonance; (b) dipole resonance
    Fig. 2. Equivalent circuit. (a) LC resonance; (b) dipole resonance
    Changes of Q-factor and absorption with different structural parameters. (a) Absorption and reflection spectra of the sensor; (b) L1; (c) L2; (d) L3; (e) W; (f) θ
    Fig. 3. Changes of Q-factor and absorption with different structural parameters. (a) Absorption and reflection spectra of the sensor; (b) L1; (c) L2; (d) L3; (e) W; (f) θ
    Effects of microfluidic channel height and thickness of cap on the sensing properties. (a) Changes of Q-factor and absorption with different microfluidic channel height; (b) changes of sensitivity with different microfluidic channel height; (c) changes of sensitivity with different thickness of cap
    Fig. 4. Effects of microfluidic channel height and thickness of cap on the sensing properties. (a) Changes of Q-factor and absorption with different microfluidic channel height; (b) changes of sensitivity with different microfluidic channel height; (c) changes of sensitivity with different thickness of cap
    Electric field distribution and surface current distribution of metal microstructure at the resonance frequency point. (a) Electric field distribution; (b) surface current distribution
    Fig. 5. Electric field distribution and surface current distribution of metal microstructure at the resonance frequency point. (a) Electric field distribution; (b) surface current distribution
    Reflectance spectra of glucose solutions with different mass fractions
    Fig. 6. Reflectance spectra of glucose solutions with different mass fractions
    MethodFrequency /THzQ-factorSensitivity /(GHz·RIU-1)
    Method in Ref. [16]0.71220
    Method in Ref. [19]1.0--1.2192
    Method in Ref. [20]0.7943--70379
    Method in Ref. [23]0.4--0.7153.17
    Proposed method0.9924313
    Table 1. Comparison of the proposed sensor with prior reported sensors
    Mass fraction ofglucose solution /%210182634
    Refractive index1.3361.3471.3601.3731.384
    Table 2. Refractive index of glucose solution with different mass fractions at 20 ℃[25]
    Zongren Li, Hu Deng, Jieping Yang, Quancheng Liu, Jin Guo, Liping Shang. High-Sensitivity Terahertz Microfluidic Sensor Based on Irregular U-type Structure[J]. Acta Optica Sinica, 2021, 41(19): 1928003
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