The Water Vapor Spectrum in the Region 8600-15 000 cm(-1): Experimental and Theoretical Studies for a New Spectral Line Database.
暂无分享,去创建一个
Jonathan Tennyson | David A. Newnham | Richard C. M. Learner | Nikolai F. Zobov | Roland Schermaul | Djedjiga Belmiloud | J. Tennyson | D. Newnham | J. Ballard | N. Zobov | R. Gary Williams | John Ballard | R. Learner | R. G. Williams | R. Schermaul | D. Belmiloud | R. G. Williams
[1] A. Calawa,et al. Tunable diode laser measurements of water vapour absorption line parameters , 1974 .
[2] Olga V. Naumenko,et al. The High-Resolution Spectrum of Water Vapor between 11 600 and 12 750 cm-1 , 1985, Journal of molecular spectroscopy.
[3] V. M. Devi,et al. Diode laser measurements of air and nitrogen broadening in the ν2 bands of HDO, H216O, and H218O , 1986 .
[4] J.-Y. Mandin,et al. H218O: line positions and intensities between 9500 and 11 500 cm−1. The (041), (220), (121), (300), (201), (102), and (003) interacting states , 1987 .
[5] 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 .
[6] Edward V. Browell,et al. Water-vapor line broadening and shifting by air, nitrogen, oxygen, and argon in the 720-nm wavelength region , 1989 .
[7] 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 .
[8] E. Browell,et al. Spectroscopy of water vapor in the 720-nm wavelength region - Line strengths, self-induced pressure broadenings and shifts, and temperature dependence of linewidths and shifts , 1989 .
[9] T. Wilkerson,et al. Water-vapor absorption line measurements in the 940-nm band by using a Raman-shifted dye laser. , 1993, Applied optics.
[10] Robert R. Gamache,et al. Collisional broadening of water vapor lines—I. A survey of experimental results , 1994 .
[11] R. Toth. Measurements of H216O line positions and strengths : 11 610 to 12 861 cm-1 , 1994 .
[12] W. B. Johnston,et al. A coolable long path absorption cell for laboratory spectroscopic studies of gases , 1994 .
[13] J. Tennyson,et al. Infrared Transition Intensities for Water: A Comparison of ab-Initio and Fitted Dipole Moment Surfaces , 1995 .
[14] J. Baker,et al. High‐resolution absorption spectra of water vapor and acetylene detected by temperature tuning of laser diodes , 1996 .
[15] Harry Partridge,et al. The determination of an accurate isotope dependent potential energy surface for water from extensive ab initio calculations and experimental data , 1997 .
[16] P. Bernath,et al. Water on the sun: line assignments based on variational calculations. , 1997, Science.
[17] Ponsardin,et al. Measurements of H216O Linestrengths and Air-Induced Broadenings and Shifts in the 815-nm Spectral Region , 1997, Journal of molecular spectroscopy.
[18] Bykov,et al. The Water Vapor Linestrengths between 11 600 and 12 750 cm-1 , 1997, Journal of molecular spectroscopy.
[19] P. Bernath,et al. Hot Bands of Water in the ν2Manifold up to 5ν2-4ν2 , 1997 .
[20] James S. Harris,et al. Laser diode cavity ring-down spectroscopy using acousto-optic modulator stabilization , 1997 .
[21] Laurence S. Rothman,et al. Reprint of: The HITRAN molecular spectroscopic database and HAWKS (HITRAN Atmospheric Workstation): 1996 edition , 1998 .
[22] O'brien,et al. Quantitative Intracavity Laser Spectroscopy Measurements with a Ti:sapphire Laser: Absorption Intensities for Water Vapor Lines in the 790-800 nm Region. , 1998, Journal of molecular spectroscopy.
[23] D. Newnham,et al. Visible absorption cross sections and integrated absorption intensities of molecular oxygen (O2 and O4) , 1998 .
[24] Robert R. Gamache,et al. New developments in the theory of pressure-broadening and pressure-shifting of spectral lines of H2O: The complex Robert-Bonamy formalism , 1998 .
[25] Zobov,et al. Water Vapor Line Assignments in the Near Infrared. , 1998, Journal of molecular spectroscopy.
[26] J. Haigh,et al. The contribution of unknown weak water vapor lines to the absorption of solar radiation , 1999 .
[27] A. A. Chursin,et al. The 1997 spectroscopic GEISA databank , 1999 .
[28] Richard C. M. Learner,et al. PRECISE LINE PARAMETERS AND TRANSITION PROBABILITY OF THE ATMOSPHERIC A BAND OF MOLECULAR OXYGEN 16O2 , 1999 .
[29] Albert Arking,et al. Bringing climate models into agreement with observations of atmospheric absorption , 1999 .
[30] V. A. Savin,et al. The near infrared, visible, and near ultraviolet overtone spectrum of water , 1999 .
[31] Jonathan Tennyson,et al. New studies of the visible and near‐infrared absorption by water vapour and some problems with the HITRAN database , 2000 .
[32] Harry Partridge,et al. Convergence testing of the analytic representation of an ab initio dipole moment function for water: Improved fitting yields improved intensities , 2000 .
[33] J. Tennyson,et al. Accurate partition function and thermodynamic data for water , 2000 .
[34] Lawrence P. Giver,et al. Visible and near-infrared H216O line intensity corrections for HITRAN-96 , 2000 .
[35] Jonathan Tennyson,et al. The Water Vapor Spectrum in the Region 8600-15 000 cm(-1): Experimental and Theoretical Studies for a New Spectral Line Database. , 2001, Journal of molecular spectroscopy.