Atmospheric methane measurement instrument using a Zeeman-split He-Ne laser.

We report the construction of an atmospheric methane measurement instrument based on a Zeeman-split IR He-Ne laser. The laser has a transverse magnetic field over ~2/3 of its gain length and can oscillate at an (unsplit) frequency (2947.91 cm(-1)) centered on a methane absorption line, or on either of two frequencies split by +/-0.055 cm(-1)) from the center, with low CH(4)) absorption. The laser is tuned to dwell sequentially at each frequency, giving two differential absorption measurements in each 46-ms tuning cycle. Atmospheric measurements are made using two multiple pass absorption cells, one with fast (0.75-s) and one with slow (5-s) flow response times. Fluctuations in ambient CH(4)) of ~20-ppb (rms, 1-s averaging) are detected, with interference fringe effects the dominant noise source. The instrument has operated in a field experiment (NASA GTE/ABLE-3A) in Alaska.

[1]  J. Drummond,et al.  Measurements of tropospheric OH concentrations: A comparison of field data with model predictions , 1987 .

[2]  S. Strahan,et al.  Nitrous oxide as a dynamical tracer in the 1987 airorne Antarctic ozone experiment , 1988 .

[3]  D. Lenschow,et al.  Direct measurements of nitrogen oxides and ozone fluxes over grassland , 1986 .

[4]  A Goldman,et al.  The HITRAN database: 1986 edition. , 1987, Applied optics.

[5]  Herwig Kogelnik,et al.  Off-Axis Paths in Spherical Mirror Interferometers , 1964 .

[6]  M. Wesely,et al.  Field measurement of small ozone fluxes to snow, wet bare soil, and lake water , 1981 .

[7]  W L Wolfe,et al.  Refractive indexes and temperature coefficients of germanium and silicon. , 1976, Applied optics.

[8]  A. Fried,et al.  Application of tunable diode laser absorption for trace stratospheric measurements of HCl: laboratory results. , 1984, Applied optics.

[9]  D. Blake,et al.  Continuing Worldwide Increase in Tropospheric Methane, 1978 to 1987 , 1988, Science.

[10]  J. A. Silver,et al.  Optical interference fringe reduction in laser absorption experiments. , 1988, Applied optics.

[11]  J. F. Butler,et al.  Tunable Diode Laser Spectroscopy: An Invited Review , 1980 .

[12]  Veerabhadran Ramanathan,et al.  Trace gas trends and their potential role in climate change , 1985 .

[13]  Gyula Molnar,et al.  A model study of the greenhouse effects due to increasing atmospheric CH4, N2O, CF2Cl2, and CFCl3 , 1985 .

[14]  C. Patel,et al.  Magnetic field tuning of gaseous laser oscillators , 1964 .

[15]  John U. White Long Optical Paths of Large Aperture , 1942 .

[16]  C. Weitkamp,et al.  Two-mirror multipass absorption cell. , 1981, Applied optics.

[17]  S. Wofsy,et al.  Tropospheric chemistry: A global perspective , 1981 .

[18]  R. Cicerone Changes in Stratospheric Ozone , 1987, Science.

[19]  B. Armstrong Spectrum line profiles: The Voigt function , 1967 .

[20]  A. S. Pine,et al.  High-resolution methane ν 3 -band spectra using a stabilized tunable difference-frequency laser system* , 1976 .

[21]  J. Wormhoudt,et al.  A measurement of the strength of the ν2 band of CH3 , 1989 .

[22]  J. Mugler,et al.  NASA global tropospheric experiment , 1983 .

[23]  D. E. Burch,et al.  Absorption of 3.39-Micron Helium–Neon Laser Emission by Methane in the Atmosphere , 1965 .

[24]  R. May,et al.  Simultaneous in situ measurements and diurnal variations of NO, NO2, O3, jNO2, CH4, H2O, and CO2 in the 40‐ to 26‐km region using an open path tunable diode laser spectrometer , 1987 .

[25]  A. J. Crawford,et al.  The global distribution of methane in the troposphere , 1987 .

[26]  Glen W. Sachse,et al.  Fast‐response, high‐precision carbon monoxide sensor using a tunable diode laser absorption technique , 1987 .