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基于微型非共振腔的石英增强光声光谱用于氦气纯度分析的实验研究
引用本文:武红鹏,董磊,郑华丹,刘研研,马维光,张雷,王五一,朱庆科,尹王保,贾锁堂. 基于微型非共振腔的石英增强光声光谱用于氦气纯度分析的实验研究[J]. 物理学报, 2013, 62(7): 70701-070701. DOI: 10.7498/aps.62.070701
作者姓名:武红鹏  董磊  郑华丹  刘研研  马维光  张雷  王五一  朱庆科  尹王保  贾锁堂
作者单位:1. 量子光学与光量子器件国家重点实验室, 山西大学激光光谱实验室, 太原 030006;2. 山西计量科学研究院, 太原 030006
基金项目:国家重点基础研究发展计划(973计划)(批准号: 2012CB921603)、 国家自然科学基金(批准号: 61275213、 61108030、 61127017、 61178009、60908019和61205216)和山西省青年科学基金(批准号: 2010021003-3、 2012021022-1)资助的课题.
摘    要:实验中设计了一种基于微型非共振腔的石英增强光声光谱痕量气体传感器, 用来检测非纯氦气中的痕量氨气浓度. 该传感器采用的微型非共振腔只在空间上限制声波扩散以达到增强信号目的, 而不是像传统微型共振腔一样依靠共振效应. 如此的设计使探测小分子无机气体的光谱测声器尺寸远远小于共振腔的配置而有利于准直. 不同气压下的信号和噪声也被研究, 用来优化传感器性能. 在这种配置下和27.7 kPa的最优气压下, 获得的最佳氨气探测灵敏度为463 ppb (1σ , 1 s积分时间), 相应的归一化噪声等效吸收系数为4.3×10-9cm-1W/√Hz.关键词:气体传感器石英增强光声光谱音叉式石英晶振类氢气体纯度分析

关 键 词:气体传感器  石英增强光声光谱  音叉式石英晶振  类氢气体纯度分析
收稿时间:2012-11-06

Purity analysis of helium using quartz-enhanced photoacoustic spectroscopy with two non-resonant micro-tubes
Wu Hong-Peng,Dong Lei,Zheng Hua-Dan,Liu Yan-Yan,Ma Wei-Guang,Zhang Lei,Wang Wu-Yi,Zhu Qing-Ke,Yin Wang-Bao,Jia Suo-Tang. Purity analysis of helium using quartz-enhanced photoacoustic spectroscopy with two non-resonant micro-tubes[J]. Acta Physica Sinica, 2013, 62(7): 70701-070701. DOI: 10.7498/aps.62.070701
Authors:Wu Hong-Peng  Dong Lei  Zheng Hua-Dan  Liu Yan-Yan  Ma Wei-Guang  Zhang Lei  Wang Wu-Yi  Zhu Qing-Ke  Yin Wang-Bao  Jia Suo-Tang
Affiliation:1. State Key Laboratory of Quantum Optics and Quantum Optics Devices, Lab for Laser Spectroscopy, Shanxi University, Taiyuan 030006, China;2. Shanxi Institute of Metrology, Taiyuan 030006, China
Abstract:A trace gas sensor, based on quartz-enhanced photoacoustic spectroscopy (QEPAS) with two non-resonant micro-tubes, was designed to detect the ammonia concentration in impure helium. Unlike the traditional micro-resonator, the non-resonant micro-tubes are used to confine the sound wave, but do not exhibit a well-defined resonant behavior. Such a design makes the dimension of the spectrophone much smaller than the micro-resonant configuration, which facilitates the optical alignment. Signal and noise, that were dependent on gas pressure, were also investigated to optimize sensor performance. With the optimal sensor parameters and the optimal gas pressure, the detection sensitivity was found to be 463 ppb (1σ , 1 s averaging time), which corresponds to the normalized absorption sensitivity of 4.3×10-9cm-1W/√Hz.
Keywords:gas sensor  quartz-enhanced photoacoustic spectroscopy  quartz tuning fork  purity analysis of hydrogen-like gas
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