Молекулярная спектроскопия Молекулярная спектроскопия
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Figure 8. Comparison of temperature dependencies for pure water vapour continuum absorption in mm-wave and mid-IR spectral ranges. Experimental data for 190 and 239 GHz are from [67] and [68], respectively; CO2 laser absorptions are from [69,70]. Solid lines show the result of calculations using formula (2a) and universal parameters n=1.63 and Do=1700 K. The data for infrared continuum (right axis) are shown in arbitrary units. The Figure is adopted from [63].

[63] Vigasin AA. Water vapor continuous absorption in various mixtures: possible role of weakly bound complexes. JQSRT 2000; 64: 25–40.
[67] Bauer A, Godon M. Temperature dependence of water vapor absorption in line wings at 190 GHz. JQSRT 1991; 46:211–20.
[68] Bauer A, Godon M, Carlier J, Ma Q. Water vapor absorption in the atmospheric window at 239 GHz. JQSRT 1995; 53:411–23.
[69] Aref’ev VN. Molecular absorption of radiation by water vapour in the relative transparency window of the atmosphere at 8–13 μm. Opt Atmos 1989; 2:1034 inRussian.
[70] Hinderling J, Sigrist MW, Kneubuhl FK. Laser-photoacoustic spectroscopy of water-vapor continuum and line absorption in the 8 to 14 μm atmospheric window. Infrared Phys 1987; 27:63–120.



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