High resolution diode laser spectroscopy of H2O spectra broadened by nitrogen and noble gases

The absorption spectra of pure H2O with mixtures of broadening gases N2, Ar, Xe, He, Ar and air have been measured in 1.39 mμ spectral region by high resolution spectrometer based on diode laser (DFB NEL, Japan). For the processing of pure water spectra and it’s mixtures with a different broadening gases in a wide pressure range we used a multispectrum fitting procedure developed at IAO. The program is based on a relatively simple Rautian-Sobel’man line profile and linear pressure dependence of the line profile parameters. H2O measured spectra bulk processing results in the retrieving of such line parameters: zero-pressure line center positions, intensities, self-broadening and self-shift coefficients of pure water, broadening and shift coefficients for other gases which are describes the experiment with the minimum residuals in a wide pressure range.

[1]  B. Parvitte,et al.  The absorption line profiles of H2O near 1.39 μm in binary mixtures with N2, O2, and H2 at low pressures , 2006 .

[2]  T. Y. Chesnokova,et al.  Spectroscopic factors, influencing the accuracy of the atmospheric radiative transfer simulation in the methane absorption bands in the near infrared region , 2013 .

[3]  Bertrand Parvitte,et al.  Diode laser spectroscopy of H2O in the 7165– range for atmospheric applications , 2002 .

[4]  A. E. Protasevich,et al.  Collision parameters of N2-broadened methane lines in R5 multiplet of 2ν3 band. Multispectrum fitting of overlapping spectral lines , 2012 .

[5]  Jean-Michel Hartmann,et al.  An isolated line-shape model to go beyond the Voigt profile in spectroscopic databases and radiative transfer codes , 2013 .

[6]  A. Solodov,et al.  Measurements of water vapor line shifts in the 8650–9020 cm−1 region caused by pressure of atmospheric gases , 2010 .

[7]  Jean-Michel Hartmann,et al.  Efficient computation of some speed-dependent isolated line profiles , 2013 .

[8]  R A Toth,et al.  Extensive measurements of H216O line frequencies and strengths: 5750 to 7965 cm(-1). , 1994, Applied optics.

[9]  A. E. Protasevich,et al.  Collisional parameters of N2 broadened methane lines in the R9 multiplet of the 2ν3 band. Multispectrum fittings of the overlapping spectral lines , 2012 .

[10]  P. Chelin,et al.  Intensities and shapes of H2O lines in the near-infrared by tunable diode laser spectroscopy , 2012 .

[11]  R. Imasu,et al.  Sensing HDO/H2O in the Ural’s atmosphere using ground-based measurements of IR solar radiation with a high spectral resolution , 2011 .

[12]  T. Y. Chesnokova,et al.  Simulation of solar radiative fluxes in the atmosphere using different models of water vapor continuum absorption in typical conditions of Western Siberia , 2013 .

[13]  S. Nabiev,et al.  Near IR TDLS study of HF first overtone line shape. I. Experimental results , 2012 .

[14]  E. R. Polovtseva,et al.  The HITRAN2012 molecular spectroscopic database , 2013 .

[15]  Peter F. Bernath,et al.  Speed-dependent Voigt profile for water vapor in infrared remote sensing applications , 2007 .

[16]  Alain Valentin,et al.  Diode-Laser Spectroscopy: Line Profiles of H2O in the Region of 1.39 μm , 2001 .

[17]  S. Mikhailenko,et al.  CRDS of water vapor at 0.1Torr between 6886 and 7406cm-1 , 2012 .

[18]  T. Gabard Calculated line broadening parameters for methane perturbed by diatomic molecules , 2013 .