2020
DOI: 10.1038/s41598-020-75076-8
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Fano resonance based defected 1D phononic crystal for highly sensitive gas sensing applications

Abstract: The defected acoustic band gap materials are promising a new generation of sensing technology based on layered cavities. We introduced a novel 1D defected phononic crystal (1D-DPC) as a high-sensitive gas sensor based on the Fano resonance transmitted window. Our designed (Lead–Epoxy) 1D-DPC multilayer has filled with a defect layer with different gases at different temperatures. In this study, Fano resonance—based acoustic band gap engineering has used to detect several gases such as O2, CO2, NH3, and CH4. Fo… Show more

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Cited by 54 publications
(17 citation statements)
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“…At resonance, the volumetric vibrations are substantially supported by plate vibrations and combine in compound bi-medium oscillators 22 . The respective peak frequency has been exploited to sense acoustic properties of the embedding fluid with high sensitivity [23][24][25] .…”
Section: In 1dmentioning
confidence: 99%
“…At resonance, the volumetric vibrations are substantially supported by plate vibrations and combine in compound bi-medium oscillators 22 . The respective peak frequency has been exploited to sense acoustic properties of the embedding fluid with high sensitivity [23][24][25] .…”
Section: In 1dmentioning
confidence: 99%
“…Thus, transmission cannot vanish in a strictly 1D structure. Reports of the vanishing of transmission in 1D structures with Fano line shapes [90,91] must therefore indicate that the samples studied are not strictly 1D. Similarly, calculations of nulls in conductance in systems containing coupled quantum dots with single channels leads [92,93] and in transmission through a cavity with a single incident and outgoing channel may arise because the interior of the system supports several internal transverse channels [37,94].…”
Section: Transmission Timementioning
confidence: 99%
“…Recent experimental and theoretical demonstrations show that high sensitivity and high-quality factor can be achieved by using different PhC sensor configurations/sensors 209,210 e.g. , PhC waveguide, 211,212 PhC nanoresonator, 213,214 PhC cavity, 215,216 polymeric PhC, 217 1-D PhC, 218,219 2-D PhC, 83,220 3-D PhC, 221 plasmonic PhC, 222 MEMS PhC, 223 porous PhC, 224 and PhC fiber. 164,225,226…”
Section: Techniques For the Improvement Of Selectivitymentioning
confidence: 99%