Changes in the Multilayer Dielectric Coating Reflection Coefficient under Variation in the Medium Humidity

[1]  L. Sinitsa,et al.  Influence of gas humidity on the reflection coefficient of multilayer dielectric mirrors. , 2016, Applied optics.

[2]  L. Sinitsa,et al.  Observation of water dimers in nanopores of silicon aerogel , 2015 .

[3]  D. Mondelain,et al.  Temperature dependence of the water vapor self‐continuum by cavity ring‐down spectroscopy in the 1.6 µm transparency window , 2014 .

[4]  Samir Kassi,et al.  The water vapour self-continuum by CRDS at room temperature in the 1.6 µm transparency window , 2013 .

[5]  Bruno Capoen,et al.  Infrared absorption by molecular gases as a probe of nanoporous silica xerogel and molecule-surface collisions: Low-pressure results , 2013 .

[6]  S. S. Vasil’chenko,et al.  High-sensitive Fourier-transform spectroscopy with short-base multipass absorption cells , 2013 .

[7]  I. V. Ptashnik,et al.  Near-infrared water vapour self-continuum at close to room temperature , 2013 .

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

[9]  H. Tanimoto,et al.  Effect of air composition (N 2 , O 2 , Ar, and H 2 O) on CO 2 and CH 4 measurement by wavelength-scanned cavity ring-down spectroscopy: calibration and measurement strategy , 2012 .

[10]  V. V. Parshin,et al.  Millimeter wave continuum absorption in moist nitrogen at temperatures 261–328 K , 2011 .

[11]  I. V. Ptashnik,et al.  Water vapour self-continuum and water dimers: 1. Analysis of recent work , 2011 .

[12]  A. Lugovskoy,et al.  Dynamic registration of the absorption spectrum of water in the SiO(2) nanopores in high-frequency range. , 2010, The Journal of chemical physics.

[13]  Rudy Peeters,et al.  Cavity enhanced absorption and cavity enhanced magnetic rotation spectroscopy , 1998 .

[14]  K. Sing,et al.  Adsorption by Powders and Porous Solids: Principles, Methodology and Applications , 1998 .

[15]  L. Rosenmann,et al.  Diode-laser measurements and calculations of CO2-line-broadening by H2O from 416 to 805 K and by N2 from 296 to 803 K , 1988 .

[16]  L. Rosenmann,et al.  Accurate calculated tabulations of IR and Raman CO(2) line broadening by CO(2), H2O, N(2), O(2) in the 300-2400-K temperature range. , 1988, Applied optics.

[17]  H. J. Bernstein,et al.  Rotation‐Vibration Spectra of Diatomic and Simple Polyatomic Molecules with Long Absorbing Paths. I. The Spectrum of Fluoroform (CHF3) from 2.4μ to 0.7μ , 1948 .