光谱学与光谱分析
光譜學與光譜分析
광보학여광보분석
SPECTROSCOPY AND SPECTRAL ANALYSIS
2015年
8期
2078-2082
,共5页
刘小利%武红鹏%邵杰%董磊%张雷%马维光%尹王保%贾锁堂
劉小利%武紅鵬%邵傑%董磊%張雷%馬維光%尹王保%賈鎖堂
류소리%무홍붕%소걸%동뢰%장뢰%마유광%윤왕보%가쇄당
石英增强光声光谱%2.0 μm分布反馈激光器%气体传感器%分子弛豫率
石英增彊光聲光譜%2.0 μm分佈反饋激光器%氣體傳感器%分子弛豫率
석영증강광성광보%2.0 μm분포반궤격광기%기체전감기%분자이예솔
Quartz-enhanced photoacoustic spectroscopy%2.0μm distributed feedback semiconductor laser%Gas sensors%Molec-ular relaxation rate
基于石英增强光声光谱技术,以中心波长为2.0μm的窄线宽分布反馈式半导体激光器(D FB )为激励光源,采用波长调制及二次谐波解调技术通过改变激光器工作电流实现波长扫描完成了痕量CO2气体检测系统,并通过优化实验参数确定了常压下激光最佳调制深度,实现了高灵敏CO2浓度的检测。通过改变待测气体中的水汽浓度,研究了水汽对CO2气体探测结果的影响,结果显示在水汽浓度低于0.2%范围内, CO2气体光声信号随H2 O浓度的上升而明显增强,当浓度高于此值后,H2 O浓度的增加对CO2光声信号的增强作用几乎维持不变。数据显示,常温常压下H2 O分子通过提高分子弛豫率最多可将二氧化碳R16吸收线的光声信号幅值提高约2.1倍。优化后的装置可以很好的实现大气中CO2浓度的检测。该装置获得的最小探测灵敏度为19 ppm(1σ,300 ms积分时间),相应的归一化噪声等效吸收系数为4.71×10-9 cm-1· W · Hz-1/2。
基于石英增彊光聲光譜技術,以中心波長為2.0μm的窄線寬分佈反饋式半導體激光器(D FB )為激勵光源,採用波長調製及二次諧波解調技術通過改變激光器工作電流實現波長掃描完成瞭痕量CO2氣體檢測繫統,併通過優化實驗參數確定瞭常壓下激光最佳調製深度,實現瞭高靈敏CO2濃度的檢測。通過改變待測氣體中的水汽濃度,研究瞭水汽對CO2氣體探測結果的影響,結果顯示在水汽濃度低于0.2%範圍內, CO2氣體光聲信號隨H2 O濃度的上升而明顯增彊,噹濃度高于此值後,H2 O濃度的增加對CO2光聲信號的增彊作用幾乎維持不變。數據顯示,常溫常壓下H2 O分子通過提高分子弛豫率最多可將二氧化碳R16吸收線的光聲信號幅值提高約2.1倍。優化後的裝置可以很好的實現大氣中CO2濃度的檢測。該裝置穫得的最小探測靈敏度為19 ppm(1σ,300 ms積分時間),相應的歸一化譟聲等效吸收繫數為4.71×10-9 cm-1· W · Hz-1/2。
기우석영증강광성광보기술,이중심파장위2.0μm적착선관분포반궤식반도체격광기(D FB )위격려광원,채용파장조제급이차해파해조기술통과개변격광기공작전류실현파장소묘완성료흔량CO2기체검측계통,병통과우화실험삼수학정료상압하격광최가조제심도,실현료고령민CO2농도적검측。통과개변대측기체중적수기농도,연구료수기대CO2기체탐측결과적영향,결과현시재수기농도저우0.2%범위내, CO2기체광성신호수H2 O농도적상승이명현증강,당농도고우차치후,H2 O농도적증가대CO2광성신호적증강작용궤호유지불변。수거현시,상온상압하H2 O분자통과제고분자이예솔최다가장이양화탄R16흡수선적광성신호폭치제고약2.1배。우화후적장치가이흔호적실현대기중CO2농도적검측。해장치획득적최소탐측령민도위19 ppm(1σ,300 ms적분시간),상응적귀일화조성등효흡수계수위4.71×10-9 cm-1· W · Hz-1/2。
A carbon dioxide (CO2 ) sensor is developed using quartz enhanced photoacoustic spectroscopy (QEPAS) with a 2.0μm distributed feedback diode laser .The detection is based on a 2 f wavelength‐modulation spectroscopy approach by dithering and scanning the laser current .The laser modulation depth is optimized at normal atmosphere pressure and room temperature . The influence of the H2 O presence in the sample gas mixture on the CO2 sensor performance is also investigated .The results show that ,with 1% CO2 concentration ,the H2 O in the concentration ranges of 0 to 0.2% has an effect on the CO2 signal ampli‐tude and phase ,and the largest amplitude difference is ~2.1 times .When the H2 O concentration is over 0.2% ,the CO2 signal amplitude is saturated and remains steady .Atmospheric CO2 concentration is well measured using the optimal sensor parame‐ters .Benefiting from the strong absorption line intensity at 4 989.97 cm -1 ,a detection limit of 19 ppm (1σ,300 ms averaging time) is achieved ,which corresponds to a normalized noise equivalent absorption coefficient of 4.71 × 10-9 cm -1 · W · Hz-1/2 .