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RAMAN SPECTROSCOPIC DEVICE AND RAMAN SPECTROSCOPIC METHOD OF AIR-WAY GAS

机译:航空气体的拉曼光谱装置和拉曼光谱方法

摘要

PURPOSE: To provide a device and a method for measuring the composition and the density of the airway gas of a patient in the Raman spectroscopic technique. CONSTITUTION: A laser beam 15 is transmitted along the longitudinal axis of a photowaveguide 13 in which a gas sample 14 is flowed, to generate Raman scattering throughout the guide. The Raman scattered light 16 is radiated from both ends of the guide 13, and is guided to a spectrometer 25 through a laser beam excluding filter 19, a lens 21, and a slit 23, as parallel rays formed by the lens 17. The spectrometer 25 comprises a grating spectrograph 27, and the spectral line guided from the slit 23, is Raman-shifted by the grating spectrograph 27. The Raman shift light 28 is dispersed to an optical sensor array 29. The optical sensor array 29 simultaneously measures the whole spetral of the Raman scattering from the mixture gas. The result of the measurement is sent to a computing means 30 to determine the relative or absolute density of the gas 14.
机译:目的:提供一种用于在拉曼光谱技术中测量患者的气道气体的成分和密度的装置和方法。组成:激光束15沿光波导13的纵轴传输,气体样本14在光波导13中流动,从而在整个光波导中产生拉曼散射。拉曼散射光16从引导件13的两端发出,并通过除滤光器19,透镜21和狭缝23之外的激光束作为由透镜17形成的平行光线被引导至光谱仪25。光谱仪。图25所示的光栅包括光栅光谱仪27,并且从狭缝23引导的光谱线被光栅光谱仪27拉曼位移。拉曼位移光28被散射到光学传感器阵列29。光学传感器阵列29同时测量整个混合气体的拉曼散射谱。测量结果被发送到计算装置30以确定气体14的相对或绝对密度。

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