Vibrational spectroscopy of the protonated water trimer provides a stringent constraint on the details of the potential energy surface (PES) and vibrational dynamics governing excess proton motion far from equilibrium. Here we report the linear spectrum of the cold, bare H(HO) ion using a two-color, IR-IR photofragmentation technique and follow the evolution of the bands with increasing ion trap temperature. The key low-energy features are insensitive to both D tagging and internal energy. The D-tagged D(DO) spectrum is reported for the first time, and the isotope dependence of the band pattern is surprisingly complex. These spectra are reproduced by large-scale vibrational configuration interaction calculations based on a new full-dimensional PES, which treat the anharmonic effects arising from large amplitude motion. The results indicate such extensive mode mixing in both isotopologues that one should be cautious about assigning even the strongest features to particular motions, especially for the absorptions that occur close to the intramolecular bending mode of the water molecule.
Serologic and molecular evidence indicates that peste des petits ruminants virus (PPRV) infection has emerged in goats and sheep in the Ngari region of southwestern Tibet, People’s Republic of China. Phylogenetic analysis confirms that the PPRV strain from Tibet is classified as lineage 4 and is closely related to viruses currently circulating in neighboring countries of southern Asia.
We
report vibrational spectra of the cryogenically cooled H9O4
+ cation along with those of the D2 tagged HD8O4
+ isotopomers
using two variations on a two-color, IR–IR double-resonance
photoexcitation scheme. The spectrum of the isolated H9O4
+ ion consists of two sharp features in the
OH stretching region that indicate exclusive formation of the “Eigen”
cation, the H3O+·(H2O)3 isomer that corresponds to the filled hydration shell around the
hydronium ion. Consistent with this structural assignment, the spectrum
of the HD8O4
+ isotopologue is resolved
into contributions from two isotopomers: one with the single OH group
on one of the three solvent water molecules and another in which it
resides on the hydronium core ion. The latter spectrum is dominated
by a broad feature assigned to the isolated hydronium OH stretching
fundamental with an envelope that is similar to that displayed by
the H3O+·(H2O)3 isotopologue.
The feature appears with a diffuse band ∼380 cm–1 above it, which is assigned to a combination band involving the
hydronium OH stretching vibration and the frustrated translation mode
of the HD2O+ core and one of the solvating water
molecules. These trends are analyzed with anharmonic calculations
involving four-mode coupling on a realistic potential surface and
interpreted in the context of vibrationally adiabatic potentials based
on insights acquired from analysis of the ground state probability
amplitudes obtained from diffusion Monte Carlo calculations.
Wet surface sightings in clusters
In principle, the surface structure of water (H
2
O) should be discernable from the O–H vibrations. In practice, however, so many configurations rapidly interconvert that the bands are bewilderingly broad. Yang
et al.
studied a cluster of 20 H
2
O surrounding a cesium ion, using isotopomers that vary in the position of one H
2
O amid 19 heavy water (D
2
O) molecules. Precisely assigned spectral features from contributing configurations mapped well onto a bulk surface spectrum.
Science
, this issue p.
275
The vibrational spectrum of the protonated water trimer, H + (H 2 O) 3 , is surprisingly complex, with many strong features in the expected region of the fundamentals associated with two H-bonded OH groups on the H 3 O + core ion. Here we follow how the bands in this region of the spectrum evolve when the energies of the fundamentals in the Hbonded OH stretches are systematically increased by the attachment of increasingly strongly bound "tag" molecules (He, Ar, D 2 , N 2 , CO, and H 2 O) to the free OH position on the hydronium core ion of H + (H 2 O) 3 , as well as by replacement of the hydrogen atom in the nonbonded OH group on hydronium with methyl and ethyl groups. This allows for the incremental transformation of the complex band pattern observed in H + (H 2 O) 3 into that of the "Eigen" structure of the protonated water tetramer. Differences among the trajectories of the various bands provide an empirical way to disentangle features primarily due to the displacements of the OH stretches bound to the hydronium core from those arising from anharmonic coupling to states involving one or more quanta in lower frequency modes. The latter are found to be dramatically enhanced when the nominal frequencies of the intermolecular OH stretching modes approach those of the intramolecular bends of the H 3 O + and H 2 O constituents in both H and D isotopologues.
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