“…3) were also observed at around 1274 and 1380 cm À1 for the vibrational frequencies of CO 2 . 26 Chen et al investigated the vibrational frequencies of CO 2 in the small and large cages of sI or sII hydrates, and their ndings are in good agreement with our results. 26 At this stage, the identication of gaseous guest molecules in the small cages of sII hydrates has been successfully demonstrated, but the types of methacrolein conformers in the large cages of sII hydrates remain unknown.…”
This study characterized new structure II (sII) clathrate hydrates, consisting of 136 H2O molecules with 8 large 51264 cages and 16 small 512 cages, with methacrolein for the first time.
“…3) were also observed at around 1274 and 1380 cm À1 for the vibrational frequencies of CO 2 . 26 Chen et al investigated the vibrational frequencies of CO 2 in the small and large cages of sI or sII hydrates, and their ndings are in good agreement with our results. 26 At this stage, the identication of gaseous guest molecules in the small cages of sII hydrates has been successfully demonstrated, but the types of methacrolein conformers in the large cages of sII hydrates remain unknown.…”
This study characterized new structure II (sII) clathrate hydrates, consisting of 136 H2O molecules with 8 large 51264 cages and 16 small 512 cages, with methacrolein for the first time.
“…The fundamental vibration band is not shown in this figure because it does not influence the shape of TPS band at Γ = 0. The anharmonicity constant of the fourth order is negative A p ≤ 0; therefore, TPS shifts to the low energy range, and the broad band of TPS is deformed in accordance with Equation . When the value A p is small, the two‐phonon band is rather wide and has two maxima of almost equal intensities on both sides (Curve 1), which reflects the density of states distribution within this two‐phonon band at one‐dimensional dispersion law.…”
Section: Fermi Resonance In the Carbon Dioxide Molecular Crystalmentioning
The vibrational spectra of a molecule and related molecular crystal are systematically analyzed theoretically with the account of the influence of anharmonic interactions between the vibrations. The specific anharmonism‐induced features in the spectra of a molecule and crystal are revealed, and spectral lineshapes at varied strength of anharmonic interaction are simulated. The proposed general theoretical approach is used for fitting the experimental vibrational spectra of CO2 substance in gas and molecular crystal phases. Pretty good coincidence of experimental data with theoretical results is demonstrated, and the constants of anharmonic interaction are obtained. The proposed theoretical approach can be used to interpret the bands in the Raman and infrared absorption spectra of various complex molecules and crystals.
“…4. The occupation of both CO 2 and N 2 molecules in the cages of sII hydrate was clearly confirmed (Table 1), but an accurate cage designation for CO 2 and N 2 was not made because CO 2 and N 2 generally do not show oneto-one correspondence between Raman shifts and hydrate cages [1,27]. However, it is reasonably expected that during the replacement, CO 2 molecules favorably attack C 3 H 8 molecules trapped in the large cages whereas N 2 molecules mainly attack CH 4 molecules captured in the small cages, considering the molecular size of the guest molecules and the dimensions of each cage.…”
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