2023
DOI: 10.1007/s12274-023-5472-x
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UV light driven high-performance room temperature surface acoustic wave NH3 gas sensor using sulfur-doped g-C3N4 quantum dots

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Cited by 33 publications
(24 citation statements)
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“…The initial and last terms in eq were pertained to the mass loading and electroacoustic/electrical conductivity effects, leading to the negative Δ f , respectively, while the middle term indicates the elastic loading effect, resulting in positive Δ f . , However, our experimental results displayed a magnificent negative Δ f under NH 3 gas, which can be ascribed to either mass loading or electrical conductivity loading effects, and thus, the elastic loading was terminated from the sensing mechanism. ,, To further explore the causes for high negative Δ f , a thin conductive film (Au ≈ 30 nm) was sputtered on the SAW sensing area prior to the addition of a ZnO@MXene layer (Figure a), because the Au thin-film-coated sensor can only detect the nonelectrical signal changes and eliminates the acoustoelectric interactions due to the shielding effect of conductive film. , According to Figure a, the Au-film-coated SAW sensor exhibited negligible Δ f to NH 3 as compared to uncoated sensor, signifying that the influence of the mass loading effect on Δ f was extremely week, and therefore, it was conferred that the negative Δ f in our results was triggered from the acoustoelectric interaction. , Furthermore, the resistive type ZnO@MXene sensor (Figure b) shows that the resistance of the sensor was reduced (conductivity increased) in the presence of NH 3 (20 ppm) with a high response of ∼39.16% as compared to the coexistence gases (Figure c), indicating the potential sensing capability of the hybrid heterostructure. The increase in sensing layer conductivity of the SAW sensor under NH 3 gas via exchanging the electron transfer leads to the attenuations in acoustic wave frequency, resulting in high negative Δ f . , …”
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confidence: 87%
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“…The initial and last terms in eq were pertained to the mass loading and electroacoustic/electrical conductivity effects, leading to the negative Δ f , respectively, while the middle term indicates the elastic loading effect, resulting in positive Δ f . , However, our experimental results displayed a magnificent negative Δ f under NH 3 gas, which can be ascribed to either mass loading or electrical conductivity loading effects, and thus, the elastic loading was terminated from the sensing mechanism. ,, To further explore the causes for high negative Δ f , a thin conductive film (Au ≈ 30 nm) was sputtered on the SAW sensing area prior to the addition of a ZnO@MXene layer (Figure a), because the Au thin-film-coated sensor can only detect the nonelectrical signal changes and eliminates the acoustoelectric interactions due to the shielding effect of conductive film. , According to Figure a, the Au-film-coated SAW sensor exhibited negligible Δ f to NH 3 as compared to uncoated sensor, signifying that the influence of the mass loading effect on Δ f was extremely week, and therefore, it was conferred that the negative Δ f in our results was triggered from the acoustoelectric interaction. , Furthermore, the resistive type ZnO@MXene sensor (Figure b) shows that the resistance of the sensor was reduced (conductivity increased) in the presence of NH 3 (20 ppm) with a high response of ∼39.16% as compared to the coexistence gases (Figure c), indicating the potential sensing capability of the hybrid heterostructure. The increase in sensing layer conductivity of the SAW sensor under NH 3 gas via exchanging the electron transfer leads to the attenuations in acoustic wave frequency, resulting in high negative Δ f . , …”
mentioning
confidence: 87%
“…3,4,14 To further explore the causes for high negative Δf, a thin conductive film (Au ≈ 30 nm) was sputtered on the SAW sensing area prior to the addition of a ZnO@MXene layer (Figure 4a), because the Au thin-filmcoated sensor can only detect the nonelectrical signal changes and eliminates the acoustoelectric interactions due to the shielding effect of conductive film. 3,14 According to Figure 4a, the Au-film-coated SAW sensor exhibited negligible Δf to NH 3 as compared to uncoated sensor, signifying that the influence of the mass loading effect on Δf was extremely week, and therefore, it was conferred that the negative Δf in our results was triggered from the acoustoelectric interaction. 3,4 Furthermore, the resistive type ZnO@MXene sensor (Figure 4b) shows that the resistance of the sensor was reduced (conductivity increased) in the presence of NH 3 (20 ppm) with a high response of ∼39.16% as compared to the coexistence gases (Figure 4c), indicating the potential sensing capability of the hybrid heterostructure.…”
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confidence: 99%
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