LIU Yang1, WU Jia-nan4, CHEN Mei-mei1, YANG Xin-hua2*, CHEN Chen3*
1. College of Communication Engineering, Jilin University, Changchun 130012, China 2. State Key Laboratory of Integrated Optoelectronics, College of Electronic Science and Engineering, Jilin University, Changchun 130012, China 3. College of Instrumentation & Electrical Engineering, Jilin University, Changchun 130061, China 4. College of Computer Science and Technology, Changchun University, Changchun 130022, China
Abstract:Methane is a colorless, odorless, flammable and explosive gas, which not only is the cause to induce significant security risk in coal mining operation, but also one of the important greenhouse gases, so the monitoring of methane is extremely critical. A trace methane gas sensor is designed and developed using the combination of tunable diode laser absorption spectroscopy (TDLAS) and wavelength modulation spectroscopy (WMS) detection technology, which is based on the methane R(3) absorption branch in 2v3 second harmonic band. Through tuning parameters -0.591 cm-1·K-1, using the method that change the working temperature of distributed feedback (DFB) laser to obtain the best absorption wavelength of methane at 1.654 μm. When the mid-wavelength of DFB laser is selected, the appropriate emitting intension can be obtained via adjusting the amplitude of inject current of DFB laser. Meanwhile, combining the frequency modulation technology to move the bandwidth of detection signal from low frequency to high frequency to reduce the 1/f noise. With aspect to the optical structure, utilizing herriott cell with 76 m effective optical path to guarantee the detection of trace methane is successful. Utilizing the proposed trace methane sensor to extract the second harmonic signal of detected methane in the range of 50 to 5 000 μmol·mol-1, and adopting minimum mean square error criterion to fit the relationship between methane concentration and signal noise ratio, harmonic peak signal and methane concentration, respectively. In addition, the minimum detection limit is 1.4 μmol·mol-1. The experiment results show the symmetry of harmonic waveform is good, no intensity modulation, and the factor of intensity-modulated impacts on harmonic detection is eliminated.
[1] Tittel F K, Dong L, Lewicki R, et al. Conference on Lasers and Electro-Optics/Pacific Rim. Optical Society of America, 2011. [2] Chen C, Newcomb R N, Wang Y D. Appl. Phys. B, 2013, 111(3): 495. [3] Chan K, Ito H, Inaba H, et al. Applied Optics, 1984, 23(19): 3415. [4] Dong L, Lewicki R, Liu R, et al. Appl. Phys. B, 2010, 107(2): 275. [5] Hegenbarth R, Steinmann A, Sarkisov S, et al. Optics Letters, 2012, 37(17): 3513. [6] Ye W L, Zheng C T, Yu X, et al. Sensors and Actuators B: Chemical, 2011, 155(1): 37. [7] McManus J B, Zahniser M S, Nelson D D. Applied Optics, 2011, 50(4): A74. [8] Northern J H, Thompson A W J, Hamilton M L, et al. Appl. Phys. B, 2013: 1. [9] CHEN Chen, HUANG Jian-qiang, Lü Mo, et al(陈 晨, 黄渐强, 吕 墨, 等). Journal of Jilin University·Engineering and Technology Edition(吉林大学学报·工学版), 2011, 41(6): 1738. [10] Roller C, Kosterev A A, Tittel F K, et al. Optics Letters, 2003, 28(21): 2052. [11] Tuzson B, Zeeman M J, Zahniser M S, et al. Infrared Physics & Technology, 2008, 51(3): 198. [12] CHEN Chen, WANG Biao, LI Chun-guang, et al(陈 晨, 王 彪, 李春光, 等). Spectroscopy and Spectral Analysis(光谱学与光谱分析), 2014, 34(3): 838.