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基于光声光谱法,利用长波、高功率、宽可调谐、单纵模固态激光器进行超高灵敏度双气体检测。

Ultra-highly sensitive dual gases detection based on photoacoustic spectroscopy by exploiting a long-wave, high-power, wide-tunable, single-longitudinal-mode solid-state laser.

作者信息

Qiao Shunda, He Ying, Sun Haiyue, Patimisco Pietro, Sampaolo Angelo, Spagnolo Vincenzo, Ma Yufei

机构信息

National Key Laboratory of Laser Spatial Information, Harbin Institute of Technology, Harbin, China.

PolySense Lab, Dipartimento Interateneo di Fisica, University and Politecnico of Bari, Via Amendola, Bari, Italy.

出版信息

Light Sci Appl. 2024 May 1;13(1):100. doi: 10.1038/s41377-024-01459-5.

DOI:10.1038/s41377-024-01459-5
PMID:38693126
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11063167/
Abstract

Photoacoustic spectroscopy (PAS) as a highly sensitive and selective trace gas detection technique has extremely broad application in many fields. However, the laser sources currently used in PAS limit the sensing performance. Compared to diode laser and quantum cascade laser, the solid-state laser has the merits of high optical power, excellent beam quality, and wide tuning range. Here we present a long-wave, high-power, wide-tunable, single-longitudinal-mode solid-state laser used as light source in a PAS sensor for trace gas detection. The self-built solid-state laser had an emission wavelength of ~2 μm with Tm:YAP crystal as the gain material, with an excellent wavelength and optical power stability as well as a high beam quality. The wide wavelength tuning range of 9.44 nm covers the absorption spectra of water and ammonia, with a maximum optical power of ~130 mW, allowing dual gas detection with a single laser source. The solid-state laser was used as light source in three different photoacoustic detection techniques: standard PAS with microphone, and external- and intra-cavity quartz-enhanced photoacoustic spectroscopy (QEPAS), proving that solid-state laser is an attractive excitation source in photoacoustic spectroscopy.

摘要

光声光谱技术(PAS)作为一种高灵敏度和高选择性的痕量气体检测技术,在许多领域有着极其广泛的应用。然而,目前光声光谱技术中使用的激光源限制了其传感性能。与二极管激光器和量子级联激光器相比,固态激光器具有光功率高、光束质量好和调谐范围宽等优点。在此,我们展示了一种长波、高功率、宽可调谐、单纵模固态激光器,用作光声光谱传感器中痕量气体检测的光源。自行搭建的固态激光器以Tm:YAP晶体作为增益介质,发射波长约为2μm,具有出色的波长和光功率稳定性以及高光束质量。9.44nm的宽波长调谐范围覆盖了水和氨的吸收光谱,最大光功率约为130mW,可实现单激光源双气体检测。该固态激光器被用作三种不同光声检测技术的光源:带麦克风的标准光声光谱技术、外腔和内腔石英增强光声光谱技术(QEPAS),证明了固态激光器是光声光谱中一种有吸引力的激发源。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/2b273261347f/41377_2024_1459_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/9c51a028e165/41377_2024_1459_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/9f567bfd91eb/41377_2024_1459_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/3bd1ee76a580/41377_2024_1459_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/e035356e4f0c/41377_2024_1459_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/a3e50be23613/41377_2024_1459_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/1d9aaec9b1eb/41377_2024_1459_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/6d4909015da3/41377_2024_1459_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/2ba80410e916/41377_2024_1459_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/c0629170f981/41377_2024_1459_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/7d3f864e4eb3/41377_2024_1459_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/bc88835dcf11/41377_2024_1459_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/10ca9c08d08c/41377_2024_1459_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/2b273261347f/41377_2024_1459_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/9c51a028e165/41377_2024_1459_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/9f567bfd91eb/41377_2024_1459_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/3bd1ee76a580/41377_2024_1459_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/e035356e4f0c/41377_2024_1459_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/a3e50be23613/41377_2024_1459_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/1d9aaec9b1eb/41377_2024_1459_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/6d4909015da3/41377_2024_1459_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/2ba80410e916/41377_2024_1459_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/c0629170f981/41377_2024_1459_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/7d3f864e4eb3/41377_2024_1459_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/bc88835dcf11/41377_2024_1459_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/10ca9c08d08c/41377_2024_1459_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/80fc/11063167/2b273261347f/41377_2024_1459_Fig13_HTML.jpg

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