Design and structural optimization of T-resonators for highly sensitive photoacoustic trace gas detection

微量气体 光声光谱学 材料科学 灵敏度(控制系统) 光学 噪音(视频) 谐振器 吸收(声学) 宽带 降噪 物理 光电子学 激光器 声学 计算机科学 电子工程 人工智能 气象学 图像(数学) 工程类
作者
Lixian Liu,Huiting Huan,Andreas Mandelis,Le Zhang,Chengfei Guo,Wei Li,Xueshi Zhang,Xukun Yin,Xiaopeng Shao,Duantian Wang
出处
期刊:Optics and Laser Technology [Elsevier BV]
卷期号:148: 107695-107695 被引量:36
标识
DOI:10.1016/j.optlastec.2021.107695
摘要

Thanks to the available ultra-wide wavelength range compared with broadband laser sources, the use of blackbody radiators in photoacoustic spectroscopy features the simultaneous detection of multiple gas species in the presence of cross-interfering absorption lines. The major problem associated with broadband incoherent sources is less power and less stable intensity per wavenumber than lasers and leads to limited gas detection sensitivity. In this paper, the detectivity of a broadband double optical path differential photoacoustic system was enhanced with the development of dimension-optimized high-responsivity T-resonators for simultaneous multiple trace gas detection. Enhanced Q-factor and external noise suppression level constitute dual criteria for the optimization of T-resonators. Three digital signal processing algorithms were separately investigated which further improved gas dectectability. The capability of the multiple–trace-gas detection framework was verified by measuring CO2, C2H2 and H2O simultaneously. The spectral results processed by a wavelet denoising algorithm present the best performance in terms of background noise suppression and spectral feature fidelity. [Q2.2] With the absorption enhancement of the optimized T-cells and background suppression of the wavelet denoising algorithm, a broadband differential photoacoustic system was achieved with only a 30 mW globar source and normalized noise equivalent absorption coefficient value of 4.1 × 10−10 W·cm−1·Hz−1/2 which is two orders of magnitude improvement over the original T-cell-based photoacoustic configuration. The noise equivalent detection limits were found to be 223 ppbv for CO2, 625 ppbv for C2H2 and 865 ppbv for H2O, respectively.
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