Infrared absorption by molecular gases as a probe of nanoporous silica xerogel and molecule-surface collisions: Low-pressure results

Transmission spectra of gases confined (but not adsorbed) within the pores of a 1.4-cm-thick silica xerogel sample have been recorded between 2.5 and 5 μm using a high-resolution Fourier transform spectrometer. This was done for pure CO, CO2, N2O, H2O, and CH4 at room temperature and pressures of a few hectopascals. Least-squares fits of measured absorption lines provide the optical-path lengths within the confined (LC) and free (LF) gas inside the absorption cell and the half width at half maximum ΓC of the lines of the confined gases. The values of LC and LF retrieved using numerous transitions of all studied species are very consistent. Furthermore, LC is in satisfactory agreement with values obtained from independent measurements, thus showing that reliable information on the open porosity volume can be retrieved from an optical experiment. The values of ΓC, here resulting from collisions of the molecules with the inner surfaces of the xerogel pores, are practically independent of the line for each gas and inversely proportional to the square root of the probed-molecule molar mass. This is a strong indication that, for the studied transitions, a single collision of a molecule with a pore surface is sufficient to change its rotational state. A previously proposed simple model, used for the prediction of the line shape, leads to satisfactory agreement with the observations. It also enables a determination of the average pore size, bringing information complementary to that obtained from nitrogen adsorption porosimetry. © 2013 American Physical Society.

[1]  V. Boudon,et al.  Experimental IR study and ab initio modelling of ethylene adsorption in a MFI-type host zeolite , 2009 .

[2]  Jean-Michel Hartmann,et al.  Model, software and database for line-mixing effects in the ν3 and ν4 bands of CH4 and tests using laboratory and planetary measurements—I: N2 (and air) broadenings and the earth atmosphere , 2006 .

[3]  P. Chelin,et al.  Abinitiocalculations of the spectral shapes of CO2isolated lines including non-Voigt effects and comparisons with experiments , 2013 .

[4]  A. Solodov,et al.  IR spectroscopy of water vapor confined in nanoporous silica aerogel. , 2010, Optics express.

[5]  L. Brown,et al.  Self-broadened 12C16O line shapes in the v=2←0 band , 2003 .

[6]  C. Frankenberg,et al.  The 2ν_3 band of CH_4 revisited with line mixing: Consequences for spectroscopy and atmospheric retrievals at 1.67 μm , 2010 .

[7]  L. Bigot,et al.  From porous silica xerogels to bulk optical glasses: The control of densification , 2010 .

[8]  J. Hartmann,et al.  Velocity effects on the shape of pure H2O isolated lines: complementary tests of the partially correlated speed-dependent Keilson-Storer model. , 2013, The Journal of chemical physics.

[9]  H. Tran,et al.  A pure H2O isolated line-shape model based on classical molecular dynamics simulations of velocity changes and semi-classical calculations of speed-dependent collisional parameters. , 2012, The Journal of chemical physics.

[10]  M. Thommes Physical Adsorption Characterization of Nanoporous Materials , 2010 .

[11]  Christopher Matranga,et al.  Trapped CO2 in Carbon Nanotube Bundles , 2003 .

[12]  J. Drummond,et al.  Temperature dependence of self- and N2-broadeningand pressure-induced shifts in the 3←0 band of CO , 2004 .

[13]  V. Boudon,et al.  Stark spectrum simulation for X2Y4 molecules: application to the ν12 band of ethylene in a high-silica zeolite. , 2012, The Journal of chemical physics.

[14]  E. Garrone,et al.  Variable temperature infrared spectroscopy: a convenient tool for studying the thermodynamics of weak solid-gas interactions. , 2005, Chemical Society reviews.

[15]  E. Teller,et al.  ADSORPTION OF GASES IN MULTIMOLECULAR LAYERS , 1938 .

[16]  S. Geschwind,et al.  BROADENING OF MICROWAVE ABSORPTION LINES DUE TO WALL COLLISIONS , 1953 .

[17]  Stefan Andersson-Engels,et al.  High sensitivity gas spectroscopy of porous, highly scattering solids. , 2008, Optics letters.

[18]  Stefan Andersson-Engels,et al.  Concentration measurement of gas embedded in scattering media by employing absorption and time-resolved laser spectroscopy. , 2002, Applied optics.

[19]  J. Yates,et al.  Vibrational behavior of adsorbed CO2 on single-walled carbon nanotubes. , 2004, The Journal of chemical physics.

[20]  D. Avnir,et al.  Recommendations for the characterization of porous solids (Technical Report) , 1994 .

[21]  Qiang Xu Nanoporous Materials : Synthesis and Applications , 2013 .

[22]  Tomas Svensson,et al.  Pore size assessment based on wall collision broadening of spectral lines of confined gas: experiments on strongly scattering nanoporous ceramics with fine-tuned pore sizes , 2013 .

[23]  Tomas Svensson,et al.  Laser spectroscopy of gas confined in nanoporous materials , 2009, 0907.5092.

[24]  R. L. Hawkins,et al.  Energy levels, intensities, and linewidths of atmospheric carbon dioxide bands , 1992 .

[25]  Tomas Svensson,et al.  Disordered, strongly scattering porous materials as miniature multipass gas cells. , 2010, Physical review letters.

[26]  Wall-collision line broadening of molecular oxygen within nanoporous materials , 2011 .

[27]  M. Lepère Self-broadening coefficients in the ν4 band of CH4 by diode-laser spectroscopy , 2006 .

[28]  J. Hartmann,et al.  Experimental and theoretical study of line mixing in methane spectra. I. The N2-broadened ν3 band at room temperature , 1999 .

[29]  M. Ducloy,et al.  Saturation effects in the sub-Doppler spectroscopy of Cesium vapor confined in an Extremely Thin Cell , 2007, 0706.0837.

[30]  D. Hurtmans,et al.  Line shape parameters measurement and computations for self-broadened carbon dioxide transitions in the 30012 ← 00001 and 30013 ← 00001 bands, line mixing, and speed dependence , 2007 .

[31]  Dimitar Slavov,et al.  Sub-Doppler spectroscopy of cesium vapor layers with nanometric and micrometric thickness , 2009 .

[32]  A. Luiten,et al.  High-resolution two-photon spectroscopy of rubidium within a confined geometry , 2013 .

[33]  G. Wlodarczak,et al.  N2- and O2-broadening coefficients and profiles for millimeter lines of 14N2O , 2003 .

[34]  P. Wagner,et al.  Line broadening and relaxation of three microwave transitions in ammonia by wall and intermolecular collisions , 1981 .

[35]  G. Rauhut,et al.  FTIR measurements and quantum chemical calculations of ethylene adsorbed on CuNaY , 2002 .

[36]  Sune Svanberg,et al.  Combined optical porosimetry and gas absorption spectroscopy in gas-filled porous media using diode-laser-based frequency domain photon migration , 2012 .

[37]  Sune Svanberg,et al.  Laser absorption spectroscopy of water vapor confined in nanoporous alumina: wall collision line broadening and gas diffusion dynamics. , 2010, Optics express.

[38]  Jean-Michel Hartmann,et al.  Collisional broadening and spectral shapes of absorption lines of free and nanopore-confined O-2 gas , 2013 .

[39]  E. C. D. Lara Electric field effect on molecules: Relation between the orientation of the molecule with respect to the field and the vibrational frequency shift observed in IR spectra of molecules adsorbed in zeolites , 1999 .