Molecular dynamics simulation of liquid methanol. II. Unified assignment of infrared, raman, and sum frequency generation vibrational spectra in methyl C–H stretching region Available to Purchase

Vibrational spectra of methyl C–H stretching region are notoriously complicated, and thus a theoretical method of systematic assignment is strongly called for in condensed phase. Here we develop a unified analysis method of the vibrational spectra, such as infrared (IR), polarized and depolarized Raman, and ssp polarized sum frequency generation (SFG), by flexible and polarizable molecular dynamics simulation. The molecular model for methanol has been developed by charge response kernel model to allow for analyzing the methyl C–H stretching vibrations. The complicated spectral structure by the Fermi resonance has been unraveled by empirically shifting potential parameters, which provides clear information on the coupling mechanism. The analysis confirmed that for the IR, polarized Raman, and SFG spectra, two-band structure at about 2830 and 2950 |$\mathrm{cm}^{-1}$|$cm −1$ results from the Fermi resonance splitting of the methyl C–H symmetric stretching and bending overtones. In the IR spectrum, the latter, higher-frequency band is overlapped with prominent asymmetric C–H stretching bands. In the depolarized Raman spectrum, the high frequency band at about 2980 |$\mathrm{cm^{-1}}$|$cm −1$ is assigned to the asymmetric C–H stretching mode. In the SFG spectrum, the two bands of the splitted symmetric C–H stretching mode have negative amplitudes of imaginary nonlinear susceptibility |$\chi ^{(2)}$|$χ(2)$⁠, while the higher-frequency band is partly cancelled by positive imaginary components of asymmetric C–H stretching modes.