2019
DOI: 10.3390/nano9111587
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Highly Sensitive Plasmonic Sensor Based on a Dual-Side Polished Photonic Crystal Fiber for Component Content Sensing Applications

Abstract: A plasmonic sensor based on a dual-side polished photonic crystal fiber operating in a telecommunication wavelength range is proposed and investigated numerically by the finite element method (FEM). We study the effects of structural parameters on the sensor’s performance and analyze their tuning effects on loss spectra. As a result, two configurations are found when the analyte refractive index (RI) changes from 1.395 to 1.415. For configuration 1, an RI resolution of 9.39 × 10−6, an average wavelength sensit… Show more

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Cited by 55 publications
(33 citation statements)
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“…The sensing performance of the sensor can be evaluated by wavelength sensitivity (wavelength interrogation) and amplitude sensitivity (amplitude interrogation) [ 5 , 10 , 15 , 18 , 26 ]. The wavelength sensitivity can be calculated from the following equation [ 5 , 10 , 11 , 12 , 13 , 14 , 15 , 17 , 18 , 19 , 20 , 26 , 37 , 38 ]: where Δ λ peak is the shift of the resonance wavelength and Δ n a is the variation of n a . As shown by the blue solid and dashed lines in Figure 3 b, we observed Δ λ peak of 15 nm when n a was varied from 1.44 to 1.45.…”
Section: Simulation Results and Discussionmentioning
confidence: 99%
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“…The sensing performance of the sensor can be evaluated by wavelength sensitivity (wavelength interrogation) and amplitude sensitivity (amplitude interrogation) [ 5 , 10 , 15 , 18 , 26 ]. The wavelength sensitivity can be calculated from the following equation [ 5 , 10 , 11 , 12 , 13 , 14 , 15 , 17 , 18 , 19 , 20 , 26 , 37 , 38 ]: where Δ λ peak is the shift of the resonance wavelength and Δ n a is the variation of n a . As shown by the blue solid and dashed lines in Figure 3 b, we observed Δ λ peak of 15 nm when n a was varied from 1.44 to 1.45.…”
Section: Simulation Results and Discussionmentioning
confidence: 99%
“…The mode characteristics and the sensing performance of the proposed sensor were simulated through commercially available software COMSOL. A perfectly matched layer (PML) was added to the outer computational region, which was applied to absorb scattered light [ 9 , 10 , 15 , 16 , 18 , 19 , 25 , 26 , 27 , 28 , 29 , 31 , 36 , 37 , 38 ].…”
Section: Structure Design and Principlementioning
confidence: 99%
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“…The RI of the air was set to 1. The fluoride phosphate (FP) N-FK51A glass was selected as the background material in our design, and its Sellmeier model [ 21 , 22 ] in the investigated wavelength range (1.40–1.75 μm) can be given by: where A 1 = 0.971247817, A 2 = 0.219014, A 3 = 0.9046517; B 1 = 0.00472302 μm 2 , B 2 = 0.01535756 μm 2 , B 3 = 168.68133 μm 2 , and λ is the operating wavelength in the vacuum (in μm).…”
Section: Modeling and Theorymentioning
confidence: 99%
“…For example, Kim et al [17] used graphene as a substitute material for Au or Ag in SPR sensors and synthesized multilayer graphene films on Ni substrates to develop fiber optic sensors with increased sensitivity. In terms of optical fiber sensing, due to the advantages of the flexible design of the PCF structure and the high sensitivity of SPR sensing technology [18], [19], the sensitivity and precision of PCR-SPR sensors are higher than those of conventional fiber optic sensors. P. B. Bing et al [20] prepared a PCF-SPR temperature sensor using a high-refractive-index glycerol liquid, achieving a low-temperature resolution as low as 4 × 10 −6 RIU.…”
Section: Introductionmentioning
confidence: 99%