2016
DOI: 10.1063/1.4945424
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Theoretical study of vibrational energy transfer of free OH groups at the water-air interface

Abstract: Recent experimental studies have shown that the vibrational dynamics of free OH groups at the water-air interface is significantly different from that in bulk water. In this work, by performing molecular dynamics simulations and mixed quantum/classical calculations, we investigate different vibrational energy transfer pathways of free OH groups at the water-air interface. The calculated intramolecular vibrational energy transfer rate constant and the free OH bond reorientation time scale agree well with the ex… Show more

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Cited by 4 publications
(3 citation statements)
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“…Thus, we used IRRAS to spectrally probe the OH stretching (ν­(OH), ∼3000–3800 cm –1 ) modes of the headgroups and their hydration shells as well as the HOH bending (δ­(HOH), ∼1500–1800 cm –1 ) modes of the hydrating water molecules. We also probed the ν­(OD) modes of dilute HOD to remove resonant vibrational excitation transfer, a Förster transfer mechanism mediated by transition dipole moment coupling; the ν­(OD) modes thus act as uncoupled local modes for more reliable reporting of water structure. ,, All spectra were collected at 21.0 ± 0.5 and 1.0 ± 1.0 °C. Shifts in the OH and OD stretching region spectra as a function of temperature were quantified by Gaussian peak fitting (Figures S3, S4, S7, S8).…”
Section: Resultsmentioning
confidence: 99%
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“…Thus, we used IRRAS to spectrally probe the OH stretching (ν­(OH), ∼3000–3800 cm –1 ) modes of the headgroups and their hydration shells as well as the HOH bending (δ­(HOH), ∼1500–1800 cm –1 ) modes of the hydrating water molecules. We also probed the ν­(OD) modes of dilute HOD to remove resonant vibrational excitation transfer, a Förster transfer mechanism mediated by transition dipole moment coupling; the ν­(OD) modes thus act as uncoupled local modes for more reliable reporting of water structure. ,, All spectra were collected at 21.0 ± 0.5 and 1.0 ± 1.0 °C. Shifts in the OH and OD stretching region spectra as a function of temperature were quantified by Gaussian peak fitting (Figures S3, S4, S7, S8).…”
Section: Resultsmentioning
confidence: 99%
“…More specifically, changes in temperature alter the transition dipole moment strengths and hydrogen-bonding configurations of the interfacial water molecules, thereby shifting the distribution of resonant vibrational frequencies. Others have shown that an increase in temperature induces a frequency mismatch between the stretch fundamental and the bending overtone of bulk water, leading to a decrease in the Fermi resonance intramolecular coupling at ∼3250 cm –1 . Intramolecular coupling dominates the vibrational relaxation pathways in interfacial water. , Thus, intramolecular coupling is possibly driving the temperature-dependent spectral shifts observed in Figure a, but the exact mechanisms responsible for these spectral shifts are currently unknown. Vibrational coupling to octadecanol- d 37 vibrational modes is also possible. , Additionally, it is nontrivial to distinguish between peak intensity contributions caused by changes in hydration shell number density and structure versus changes in transition dipole moment strength as a function of temperature, further complicating the spectral interpretation.…”
Section: Resultsmentioning
confidence: 99%
“…From a theoretical point of view, the SFG spectrum is a second-order susceptibility that arises from the interactions between the incident electric fields and the molecules. Both the real and imaginary parts of the appropriate susceptibility can be obtained using the Fourier–Laplace transform of a time-correlation function ( 11 , 14 , 16 , 17 , 27 33 ). Often, the water structures for deriving the susceptibility are calculated using a molecular dynamics (MD) simulation.…”
mentioning
confidence: 99%