Fiber optic photoacoustic gas sensor enhanced by multi-pass cell with overlapping phantom spots

A neotype fiber optic photoacoustic gas sensor with overlapping phantom spots based multi-pass is proposed, which greatly improves the reflection times and the length of gas absorption path. Moreover, the detection accuracy of photoacoustic spectroscopy (PAS) system is independent of the optical int...

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Veröffentlicht in:Sensors and actuators. B, Chemical Chemical, 2024-08, Vol.412, p.135816, Article 135816
Hauptverfasser: Zhao, Xinyu, Wang, Heng, Qi, Hongchao, Xu, Yufu, Guo, Min, Chen, Ke
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Sprache:eng
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Zusammenfassung:A neotype fiber optic photoacoustic gas sensor with overlapping phantom spots based multi-pass is proposed, which greatly improves the reflection times and the length of gas absorption path. Moreover, the detection accuracy of photoacoustic spectroscopy (PAS) system is independent of the optical interference effect caused by overlapping spots, which is different from tunable diode laser absorption spectroscopy (TDLAS) technology. A mathematical model including light beam motion space, spot size and overlap discrimination of multi-pass structure based on overlapping phantom spots is established. The incident light is reflected up to dozens of times in the resonator with a diameter of only 8 mm. The emergent light does not need to converge on a photodetector, which reduces the difficulty of adjusting the optical path and promotes the realization of overlapping phantom spots. The experimental results show that the amplitude of photoacoustic signal is improved by about 40 times compared with the single spot structure. Appling high-sensitivity optical fiber cantilever to detect the sound pressure signal. The detection limit of C2H2 gas reaches 8.2 ppt. The normalized noise equivalent absorption (NNEA) coefficient of the gas sensor is achieved to be 9.3×10−11 cm−1WHz−1/2. •A neotype fiber optic photoacoustic gas sensor with overlapping phantom spots based multi-pass is proposed.•The influence of optical interference effect caused by overlapping spots in TDLAS technology is avoided.•The incident light is reflected up to dozens of times in the resonator with a diameter of only 8 mm.•The detection limit of C2H2 gas reaches 8.2 ppt and the NNEA coefficient is 9.3×10-11 cm-1WHz-1/2.
ISSN:0925-4005
1873-3077
DOI:10.1016/j.snb.2024.135816