2018
DOI: 10.1016/j.optlastec.2017.12.003
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[INVITED] Surface plasmon cavities on optical fiber end-facets for biomolecule and ultrasound detection

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Cited by 27 publications
(13 citation statements)
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“…We demonstrate in Supporting Information S1 that the second-order harmonic comes from the narrow width of the nanoslit, and no bandgap at k x = 0 exists in an array with w / p = 50%. The band-edge mode at 800 nm corresponds to a dark mode, whereas the other one at 825 nm being a bright mode, as analyzed in refs . According to the generalized Bragg condition mλ laser ≈ 2 pn eff , where m is the Bragg order, λ laser is the lasing wavelength, and n eff is the effective index, our plasmonic array is essentially a second-order DFB cavity with m = 2, while the out-coupling of the SPR modes into the p -polarized photons is attributed to the first-order Fourier component of the array at a spatial frequency of 2π/ p . , As a comparison, we also calculated the band diagram of a first-order DFB structure using nanoslit arrays, which is shown in Supporting Information S2.…”
Section: Resultsmentioning
confidence: 88%
“…We demonstrate in Supporting Information S1 that the second-order harmonic comes from the narrow width of the nanoslit, and no bandgap at k x = 0 exists in an array with w / p = 50%. The band-edge mode at 800 nm corresponds to a dark mode, whereas the other one at 825 nm being a bright mode, as analyzed in refs . According to the generalized Bragg condition mλ laser ≈ 2 pn eff , where m is the Bragg order, λ laser is the lasing wavelength, and n eff is the effective index, our plasmonic array is essentially a second-order DFB cavity with m = 2, while the out-coupling of the SPR modes into the p -polarized photons is attributed to the first-order Fourier component of the array at a spatial frequency of 2π/ p . , As a comparison, we also calculated the band diagram of a first-order DFB structure using nanoslit arrays, which is shown in Supporting Information S2.…”
Section: Resultsmentioning
confidence: 88%
“…The development of specific probes can effectively detect and quantify the specific protein content in body fluids, which plays an important role in drug effectiveness evaluation and disease diagnosis [ 111 ]. However, in the actual application environment, both label-free and label-assisted technology are inevitably affected by biofouling [ 112 ].…”
Section: Biomedical Applications Of Zwitterionic Hydrogelsmentioning
confidence: 99%
“…Therefore, every alteration at the sensor surface, such as changing the RI, temperature, or the binding of molecules, results in the resonant wavelength(s) shifting. According to this principle, numerous optical fiber-based RI sensors for the quantitative analysis of chemical reactions and biological interactions have been demonstrated, based on arrays of metallic nanodisks, 87 nanodots, 86,113 nanoholes, 76,77,175,176,[244][245][246] nanoslits and nanogratings, 95,174,[247][248][249] nanopillars and nanorods, 250,251 nanorings, 89 nanotrimers, 252 and metal-dielectric nanocrystals. 88,112,121 For example, Jia et al 174 constructed plasmonic optical fibers by transferring patterned metal nanostructures onto optical fiber endfaces, which showed narrow linewidths (6.6 nm) and a high figure of merit (60.7).…”
Section: D Functional Surfacesmentioning
confidence: 99%