Short-Path Near-Infrared Laser Detection of Environmental Gases by Wavelength-Modulation Spectroscopy
Authors: Isao Tomita
Abstract:
The detection of environmental gases, 12CO2, 13CO2, and CH4, using near-infrared semiconductor lasers with a short laser path length is studied by means of wavelength-modulation spectroscopy. The developed system is compact and has high sensitivity enough to detect the absorption peaks of isotopic 13CO2 of a 3-% CO2 gas at 2 μm with a path length of 2.4 m, where its peak size is two orders of magnitude smaller than that of the ordinary 12CO2 peaks. In addition, the detection of 12CO2 peaks of a 385-ppm (0.0385-%) CO2 gas in the air is made at 2 μm with a path length of 1.4 m. Furthermore, in pursuing the detection of an ancient environmental CH4 gas confined to a bubble in ice at the polar regions, measurements of the absorption spectrum for a trace gas of CH4 in a small area are attempted. For a 100-% CH4 gas trapped in a ∼ 1 mm3 glass container, the absorption peaks of CH4 are obtained at 1.65 μm with a path length of 3 mm, and also the gas pressure is extrapolated from the measured data.
Keywords: Environmental Gases, Near-Infrared Laser Detection, Wavelength-Modulation Spectroscopy.
Digital Object Identifier (DOI): doi.org/10.5281/zenodo.1096857
Procedia APA BibTeX Chicago EndNote Harvard JSON MLA RIS XML ISO 690 PDF Downloads 1749References:
[1] J. K. Casper, Greenhouse Gases: Worldwide Impacts, 1st ed., New York: Facts On File, Inc., 2010.
[2] Greenhouse Gases Factsheet, Center for Sustainable Systems, University of Michigan, 2013, Pub. No. CSS05-21.
[3] G. J. Koch, B. W. Barnes, M. Petros, J. Y. Beyon, F. Amzajerdian, J. Yu, R. E. Davis, S. Ismail, S. Vay, M. J. Kavaya, and U. N. Singh, “Coherent differential absorption lidar measurements of CO2,” Appl. Opt. 43, 2004, pp.5092-5099.
[4] A. I. Karapuzikov, A. N. Malov, and I. V. Sherstov, “Tunable TEA CO2 laser for long-range DIAL lidar,” Infrared Phys. & Tech. 41, 2000, pp.77-85.
[5] A. R. Bahrampour and A. A. Askari, “Fourier-wavelet regularized deconvolution (ForWaRD) for lidar systems based on TEA-CO2 laser,” Opt. Comm. 257, 2006, pp.97-111.
[6] K. E. Bozier, G. N. Pearson, F. Davies, and C. G. Collier, “Evaluating the precision of a transverse excitation atmospheric based CO2 Doppler lidar system with in situ sensors,” J. Opt. A: Pure Appl. Opt. 6, 2004, pp.608-616.
[7] S. D. Mayor, D. H. Lenschow, R. L. Schwiesow, J. Mann, C. L. Frush, and M. K. Simon, “Validation of NCAR 10.6-μm CO2 Doppler lidar radial velocity measurements and comparison with a 915-MHz profiler,” J. Amtos. & Ocean. Tech. 14, 1997, pp.1110-1126.
[8] D. Sakaizawa, C. Nagasawa, T. Nagai, M. Abo, Y. Shibata, M. Nakazato, and T. Sakai, “Development of a 1.6 μm differential absorption lidar with a quasi-phase-matching optical parametric oscillator and photon-counting detector for the vertical CO2 profile,” Appl. Opt. 48, 2009, pp.748-757.
[9] R. Zumbrunn, A. Neftel, and H. Oeschger, “CO2 measurements on 1-cm3 ice samples with an IR laser spectrometer (IRLS) combined with a new dry extraction device,” Earth and Planet. Sci. Lett. 60, 1982, pp.318-324.
[10] J. R. Melton, M. J. Whiticar, and P. Eby, “Stable carbon isotope ratio analyses on trace methane from ice samples,” Chemical Geology 288, 2011, pp.88-96.
[11] J. A. Silver, “Frequency-modulation spectroscopy for trace species detection: theory and comparison among experimental methods,” Appl. Opt. 31, 1992, pp.707-717.
[12] H. Li, G. B. Rieker, X. Liu, J. B. Jeffries, and R. K. Hanson, “Extension of wavelength-modulation spectroscopy to large modulation depth for diode laser absorption measurements in high-pressure gases,” Appl. Opt. 45, 2006, pp.1052-1061.
[13] G. B. Rieker, J. B. Jeffries, and R. K. Hanson, “Calibration-free wavelength-modulation spectroscopy for measurements of gas temperature and concentration in harsh environments,” Appl. Opt. 48, 2009, pp.5546-5560.
[14] K. Tanaka and K. Tonokura, “Sensitive measurements of stable carbon isotopes of CO2 with wavelength modulation spectroscopy near 2 μm,” Appl. Phys. B 105, 2011, pp.463-469. A sizable multi-path gas cell with a path length of 29.9 m is used for high-precision measurements.
[15] M. Oishi, M. Yamamoto, and K. Kasaya, “2.0-μm single-mode operation of InGaAs-InGaAsP distributed-feedback buried-heterostructure quantum-well lasers,” IEEE Photon. Tech. Lett. 9, 1997, pp.431-433.
[16] M. Mitsuhara, M. Ogasawara, M. Oishi, H. Sugiura, and K. Kasaya, “2.05-μm wavelength InGaAs-InGaAs distributed-feedback multiquantum-well lasers with 10-mW output power,” IEEE Photon. Tech. Lett. 11, 1999, pp.33-35.
[17] The products of NTT Electronics Co. The semiconductor laser diodes used in the experiments were all obtained at http://www.ntt-electronics.com/en/products/photonics/gas sensing.html
[18] The HITRAN database. http://www.cfa.harvard.edu/hitran/
[19] MOLSPEC. This software computes the transmission rate of a laser beam passing through a selected gas with a selected laser wavelength, path length, pressure, and temperature. http://www.lasercomponents.com/us/news/molspec-v-industrial/