The 1- bands and the O2 (0–1) and (1–0) X3Σg−−b1Σg+ bands in the Earth atmosphere

Abstract The CO2 triad of bands in the 9300– 9700 cm −1 region have been observed in near infrared 0.05 cm −1 resolution ground-based solar absorption spectra. This interval is a portion of spectra taken in the 9000– 12,000 cm −1 region, at large solar zenith angles. Considering the available line positions and pressure line shifts for CO2, H2O and O2 in this region as of 2000, it was concluded that these observations show significant inconsistencies among the line positions of the species as listed in the atmospheric spectroscopy databases. The spectra allow a better definition of the O2 (0–1) X3Σg−−a1Δg band, with the discrete (0–1) transitions observable in the 9300– 9450 cm −1 , superimposed on a collision-induced continuum covering the 9200– 9700 cm −1 region. This continuum, as well as the (0–0) continuum in the 7900 cm −1 region, have been previously studied only from atmospheric spectra with much lower spectral resolution. The discrete O2 (1–0) transitions of the X3Σg−−b1Σg+ atmospheric B-band are observed in the 11,500– 11,600 cm −1 region, but no evidence is found for an underlying continuum. A recent laboratory study of the 2ν 1 +3ν 3 12 CO 2 triad significantly improves the consistency between the O2, H2O and CO2 lines in the atmospheric spectra.

[1]  C. Boulet,et al.  Self‐shifting of CO2 lines in the 3ν3 band at 1.43 μm , 1980 .

[2]  V. Malathy Devi,et al.  Measurements of pressure broadening and pressure shifting by nitrogen in the 4.3-μm band of 12C16O2 , 1992 .

[3]  R. Toth Measurements of H216O line positions and strengths : 11 610 to 12 861 cm-1 , 1994 .

[4]  G. T. Fraser,et al.  Rotational Line Strengths and Self-Pressure-Broadening Coefficients for the 1.27-microm, a (1)D(g)-X (3)?(g)(-), v = 0-0 Band of O(2). , 1998, Applied optics.

[5]  Simonsen,et al.  The 0 --> 3 Overtone Band of CO: Precise Linestrengths and Broadening Parameters. , 1999, Journal of molecular spectroscopy.

[6]  Pressure-Shift of the (0,0) and (1,0) Bands of the Oxygen[formula]Transition from Fourier Transform Spectroscopy , 1995 .

[7]  Frank J. Murcray,et al.  Observed atmospheric collision‐induced absorption in near‐infrared oxygen bands , 1998 .

[8]  G. Millot,et al.  High-resolution stimulated Raman spectroscopy of O2 , 1992 .

[9]  S. Neshyba,et al.  N2 and O2 induced halfwidths and line shifts of water vapor transitions in the (301)←(000) and (221)←(000) bands , 1998 .

[10]  Guelachvili,et al.  Absolute Wavenumbers and Self-Induced Pressure Lineshift Coefficients for the 3-0 Vibration-Rotation Band of 12C16O , 1997, Journal of molecular spectroscopy.

[11]  Laurence S. Rothman,et al.  Reprint of: The HITRAN molecular spectroscopic database and HAWKS (HITRAN Atmospheric Workstation): 1996 edition , 1998 .

[12]  S. Tashkun,et al.  GLOBAL FITTING OF 12C16O2 VIBRATIONAL-ROTATIONAL LINE POSITIONS USING THE EFFECTIVE HAMILTONIAN APPROACH , 1998 .

[13]  K. Smith,et al.  Collision‐induced absorption of solar radiation in the atmosphere by molecular oxygen at 1.27 μm: Field observations and model calculations , 2001 .

[14]  Laurence S. Rothman,et al.  The HITRAN molecular spectroscopic database and HAWKS (HITRAN atmospheric workstation) , 1998, Defense, Security, and Sensing.

[15]  Nathalie Picqué,et al.  Absolute line intensities, vibrational transition moment, and self-broadening coefficients for the 3-0 band of 12 C 16 O , 2000 .

[16]  D. A. Newnham,et al.  Near‐infrared absorption cross sections and integrated absorption intensities of molecular oxygen (O2, O2‐O2, and O2‐N2) , 2000 .

[17]  V. Malathy Devi,et al.  Air- and N2-broadening coefficients and pressure-shift coefficients in the 12C16O2 laser bands , 1998 .

[18]  Nathalie Picqué,et al.  A multispectrum fitting procedure to deduce molecular line parameters: Application to the 3-0 band of 12C16O , 2001 .

[19]  J. Flaud,et al.  H216O: Line positions and intensities between 8000 and 9500 cm−1: the second hexad of interacting vibrational states: {(050), (130), (031), (210), (111), (012)} , 1988 .

[20]  Edward V. Browell,et al.  Water-vapor line broadening and shifting by air, nitrogen, oxygen, and argon in the 720-nm wavelength region , 1989 .

[21]  G. Guelachvili,et al.  12C16O2 analysis of emission Fourier spectra in the 4.5-μm region: Rovibrational transitions 0v2lv3-0v2l(v3 − 1), v2 = l , 1981 .

[22]  Jean-Marie Flaud,et al.  : line positions and intensities between 9500 and 11500 cm−1. The interacting vibrational states (041), (220), (121), (022), (300), (201), (102), and (003) , 1989 .

[23]  A. A. Chursin,et al.  The 1997 spectroscopic GEISA databank , 1999 .

[24]  Yuan-Pern Lee,et al.  Wavenumbers, strengths, widths and shifts with pressure of lines in four bands of gaseous 16O2 in the systems a1Δg−X3Σg− and b1Σg+−X3Σg− , 2000 .

[25]  Lawrence P. Giver,et al.  Absolute Rovibrational Intensities and Self-Broadening and Self-Shift Coefficients for the X1Σ+V=3←V=0 Band of 12C16O , 2001 .

[26]  Laurence S. Rothman,et al.  IMPROVED SPECTRAL PARAMETERS FOR THE THREE MOST ABUNDANT ISOTOPOMERS OF THE OXYGEN MOLECULE , 1998 .

[27]  David A. Newnham,et al.  Temperature and pressure dependence of linewidths and integrated absorption intensities for the O2(a1Δg-X3Σg-) transition , 2000 .

[28]  G. Toon,et al.  Atmospheric CO2 retrieved from ground‐based near IR solar spectra , 2002 .

[29]  Alain Campargue,et al.  NOTE: The 2ν1+3ν3 Triad of 12CO2 , 2002 .

[30]  J.-Y. Mandin,et al.  Interpretation of the CO2 absorption bands observed in the Venus infrared spectrum between 1 and 2.5 μm , 1977 .

[31]  R. L. Hawkins,et al.  Energy levels, intensities, and linewidths of atmospheric carbon dioxide bands , 1992 .

[32]  Laurence S. Rothman,et al.  The HITRAN molecular spectroscopic database: edition of 2000 including updates through 2001 , 2003 .

[33]  S. Schwartz,et al.  The Atmospheric Radiation Measurement (ARM) Program: Programmatic Background and Design of the Cloud and Radiation Test Bed , 1994 .

[34]  R. Zare,et al.  Resolution of the discrepancies concerning the optical and microwave values for B0 and D0 of the X 3Σg− state of O2 , 1973 .

[35]  James B. Burkholder,et al.  Absorption measurements of oxygen between 330 and 1140 nm , 1990 .

[36]  J. Bösenberg Measurements of the pressure shift of water vapor absorption lines by simultaneous photoacoustic spectroscopy , 1985, Topical Meeting on Optical Remote Sensing of the Atmosphere.

[37]  J. Butcher The shrinking cone limit and quark spin effects in muon-induced dimuon events , 1982 .

[38]  Brown,et al.  Experimental Line Parameters of the Oxygen A Band at 760 nm. , 2000, Journal of molecular spectroscopy.