The 1- bands and the O2 (0–1) and (1–0) X3Σg−−b1Σg+ bands in the Earth atmosphere
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Laurence S. Rothman | Frank J. Murcray | A. Goldman | J.-Y. Mandin | Curtis P. Rinsland | Lawrence P. Giver | C. Rinsland | L. Rothman | L. Giver | R. R. Gamache | A. Goldman | F. Murcray | T. Stephen | J. Mandin | T. M. Stephen | R. Gamache
[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.