Pressure tuning of the Fermi resonance in liquid methanol: implications for the analysis of high-pressure vibrational spectroscopy experiments.

It has been argued that pressure tuning allows for unambiguous assignment of the nonperturbed bands involved in the Fermi coupling of molecular systems in the condensed phase. Here we study the pressure evolution of the Fermi resonance occurring in liquid methanol between the symmetric methyl-stretch fundamental and the methyl-bending overtones. Our analysis is based on Raman experiments in both stretching and bending fundamental regions, which are used to evaluate the effect of pressure on accidental degeneracies occurring in the vibrational spectra of liquid methanol. We emphasize that the difference in frequency of the Fermi doublet constitutes the governing quantity to determine the condition at which the exact degeneracy of the unperturbed modes occurs. Analysis based on the intensity ratio of the Fermi doublet must be disregarded. We confirm the necessity of measuring the full vibrational spectrum under pressure in order to obtain the Fermi coupling parameters unambiguously and to give a correct assignment of the bands involved in the resonance phenomenon. We also analyze the possible occurrence of several simultaneous resonance effects using a multilevel perturbation model. This model provides an appropriate description of the frequencies observed in the experiments over the whole pressure range if we consider that the main resonance occurs between nu3 and 2nu10, in contrast to previous assignments. Our global analysis leads to some general rules concerning measurement and interpretation of high-pressure vibrational spectroscopy experiments.

[1]  Hydrogen bonding and dynamics of methanol by high-pressure diamond-anvil cell NMR. , 2005 .

[2]  R. Meyer,et al.  Methanol and deuterated species: Infrared data, valence force field, rotamers, and conformation , 1974 .

[3]  Shiv k. Sharma,et al.  Raman spectra of methanol and ethanol at pressures up to 100 kbar , 1980 .

[4]  M. Taravillo,et al.  Diamond as pressure sensor in high‐pressure Raman spectroscopy using sapphire and other gem anvil cells , 2003 .

[5]  Zexiang Shen,et al.  Near infrared excited micro-Raman spectra of 4:1 methanol–ethanol mixture and ruby fluorescence at high pressure , 1999 .

[6]  T. W. Żerda,et al.  Fermi resonance and vibrational lineshapes of the CH3 group in liquid methanol , 1985 .

[7]  E. Bright Wilson,et al.  Book Reviews: Molecular Vibrations. The Theory of Infrared and Raman Vibrational Spectra , 1955 .

[8]  Y. H. Wu,et al.  High‐pressure Raman study of liquid and crystalline CH3F up to 12 GPa , 1995 .

[9]  Heather C. Allen,et al.  Surface studies of aqueous methanol solutions by vibrational broad bandwidth sum frequency generation spectroscopy , 2003 .

[10]  Shuliang L. Zhang,et al.  Infrared intensities of liquids XXI: integrated absorption intensities of CH3OH, CH3OD, CD3OH and CD3OD and dipole moment derivatives of methanol , 1997 .

[11]  L. Halonen Theoretical study of vibrational overtone spectroscopy and dynamics of methanol , 1997 .

[12]  G. Herzberg Infrared and raman spectra , 1964 .

[13]  Jeon,et al.  Pressure dependence of the vibron modes in solid hydrogen and deuterium. , 1992, Physical review. B, Condensed matter.

[14]  L. H. Jones,et al.  Infrared and Raman studies of pressure effects on the vibrational modes of solid CO2 , 1981 .

[15]  R. Zallen Pressure-Raman effects and vibrational scaling laws in molecular crystals: S 8 and As 2 S 3 , 1974 .

[16]  E. Meijer,et al.  Density-functional theory-based molecular simulation study of liquid methanol. , 2004, The Journal of chemical physics.

[17]  V. Astinov,et al.  Raman and IR study on the H2O - CH3OH mixed solvent at 25°C using fourier deconvolution technique , 1993 .

[18]  T. W. Żerda,et al.  Raman study of the temperature and pressure effects on the Fermi resonance and hydrogen bonding in liquid ammonia , 1984 .

[19]  R. Dixon Anomalous Band Intensity in Fermi Resonance , 1959 .

[20]  Krešimir Furić,et al.  Methanol in isolated matrix, vapor and liquid phase: Raman spectroscopic study , 1993 .

[21]  D. Ben‐Amotz,et al.  Pressure Dependent Vibrational Fermi Resonance in Liquid CH3OH and CH2Cl2 , 1998 .

[22]  M. Taravillo,et al.  Effect of pressure on hydrogen bonding in liquid methanol. , 2002, Physical review letters.

[23]  J. Jonas,et al.  High pressure chemistry, biochemistry, and materials science , 1993 .

[24]  V. Lemos,et al.  Effects of pressure on the Raman spectra of a 4:1 methanol–ethanol mixture , 1990 .

[25]  C. H. Wang,et al.  Raman study of Fermi resonance, hydrogen bonding, and molecular reorientation in liquid ammonia , 1973 .

[26]  N. Sheppard,et al.  Anharmonicity of CH3 deformation vibrations and Fermi resonance between the symmetrical CH3 stretching mode and overtones of CH3 deformation vibrations , 1972 .

[27]  John R. Ferraro,et al.  Vibrational Spectroscopy at High External Pressures , 2006 .

[28]  M. Taravillo,et al.  Phase transitions and hindered rotation in dimethylacetylene at high pressures probed by Raman spectroscopy. , 2004, The Journal of chemical physics.

[29]  Martin Schwartz,et al.  Fermi resonance in aqueous methanol , 1980 .

[30]  Michael Falk,et al.  Infrared Spectra of Methanol and Deuterated Methanols in Gas, Liquid, and Solid Phases , 1961 .