Vibrational Substructure in the OH Stretching Transition of Water and HOD
Вибрационная подсструктура в ОН-растяжении воды и HOD
2004-09-25
SCID: 54.1/n8ue9jx2
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HOD in D2OOH stretchingstretch-to-bend anharmonic couplingultrafast nonlinear vibrational spectroscopy
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Abstract (AI)
Ultrafast nonlinear vibrational spectroscopy with mid-IR pumping and incoherent anti-Stokes Raman probing is used to study v = 1 excitations of OH stretching (νOH) of water and of HOD in D2O solvent (HOD/D2O). The parent νOH decay and the appearance of daughter stretching and bending excitations are simultaneously monitored, which allows for characterization of the stretch decay pathways. At all times and with all pump frequencies within the νOH band, the excited-state spectrum can be fit by two overlapping subbands, a broader red-shifted band and a narrower blue-shifted band . We show these subbands are dynamically distinguishable. They decay with different lifetimes and evidence characteristically different decay pathways. Excitations of the subband generate bending vibrations that does not. The shorter lifetime (∼0.5 ps) of the subband compared to the subband (0.8−0.9 ps) results primarily from enhanced stretch-to-bend anharmonic coupling. The subbands represent persistent structures in the excited state, in that interconversion between subbands (2−10 ps) is slower than excited-state decay. A tentative structural interpretation is proposed. The subband, on the basis of simulations, its red shift ,and its shorter lifetime, is proposed to result from strongly hydrogen-bonded “ice-like” water. The subband has a smaller amplitude in HOD/D2O than in water, possibly because HOD has a single localized OH-stretching vibration whereas water has two delocalized stretching vibrations.
Key Findings
1
A tentative structural assignment: the red-shifted, shorter-lived subband corresponds to strongly hydrogen-bonded 'ice-like' water; the blue-shifted subband is less hydrogen-bonded.
2
Excitation of the shorter-lived red-shifted subband generates bending vibrations, whereas excitation of the other subband does not, implicating enhanced stretch-to-bend anharmonic coupling for the red-shifted component.
3
Interconversion between subbands occurs on 2–10 ps time scale, slower than excited-state decay, so subbands are persistent excited-state structures.
4
The excited-state νOH spectrum is decomposable at all pump times/frequencies into two overlapping subbands: a broader red-shifted subband and a narrower blue-shifted subband.
5
The red/blue subband amplitude differs between systems: the red-shifted subband has smaller amplitude in HOD/D2O than in H2O, possibly due to HOD having a single localized OH stretch versus water's two delocalized stretches.
6
The two subbands are dynamically distinguishable: they decay with different lifetimes (red-shifted ~0.5 ps, blue-shifted ~0.8–0.9 ps) and follow different decay pathways.
7
Ultrafast mid-IR pump and incoherent anti-Stokes Raman probing were used to monitor νOH v=1 decay and appearance of daughter stretching and bending excitations simultaneously.
Research Object
v = 1 excitations of the OH stretching (νOH) vibration in liquid water and in HOD diluted in D2O (HOD/D2O)
Research Subject
the vibrational substructure of the νOH excited-state spectrum — two dynamically distinguishable overlapping subbands (red-shifted broader and blue-shifted narrower), their distinct lifetimes, decay pathways (stretch-to-bend anharmonic coupling and generation of daughter modes), interconversion dynamics, and structural assignments relating subbands to hydrogen-bonding environments
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2004-09-25
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