A hydroxyl radical detection system using gas expansion and fast gating laser-induced fluorescence techniques |
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Authors: | Hao Chen Renzhi Hu Pinhua Xie Xingbiao Xing Liuyi Ling Zhiyan Li Fengyang Wang Yihui Wang Jianguo Liu Wenqing Liu |
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Institution: | 1 Department of Precision Machinery and Precision Instrumentation, University of Science and Technology of China, Hefei 230027, China;2 Key Laboratory of Environmental Optics and Technology, Anhui Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Hefei 230031, China;3 CAS Center for Excellence in Regional Atmospheric Environment, Institute of Urban Environment, Chinese Academy of Sciences, Xiamen 361000, China;4 Institute of Electric and Information Technology, Anhui University of Science and Technology, Huainan 232001, China |
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Abstract: | An OH radical measurement instrument based on Fluorescence Assay by Gas Expansion (FAGE) has been developed in our laboratory. Ambient air is introduced into a low-pressure fluorescence cell through a pinhole aperture and irradiated by a dye laser at a high repetition rate of 8.5 kHz. The OH radical is both excited and detected at 308 nm using A-X(0,0) band. To satisfy the high efficiency needs of fluorescence collection and detection, a 4-lens optical system and a self-designed gated photomultiplier (PMT) is used, and gating is actualized by switching the voltage applied on the PMT dynodes. A micro channel photomultiplier (MCP) is also prepared for fluorescence detection and can interchange with the gated PMT. Then the weak signal is accumulated by a photon counter in a specific timing. The OH radical excitation spectrum range in the wavelength of 307.82–308.2 nm is detected and the excited line for OH detection is determined to be Q1(2) line. The calibration of the FAGE system is researched by using simultaneous photolysis of H2O and O2. The minimum detection limit of the instrument using gated PMT is determined to be 9.4 × 105 molecules/cm3, and the sensitivity is 9.5 × 10− 7 cps/(OH·cm− 3), with a signal-to-noise ratio of 2 and an integration time of 60 sec, while OH detection limit and the detection sensitivity using MCP is calculated to be 1.6 × 105 molecules/cm3 and 2.3 × 10− 6 cps/(OH·cm− 3). The laboratory OH radical measurement is carried out and results show that the proposed system can be used for atmospheric OH radical measurement. |
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Keywords: | OH radical Laser-induced fluorescence Fluorescence assay by gas expansion Photomultiplier Photon counting |
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