4.8 Article

Structural and Electric Field Effects of Ions in Aqueous Nanodrops

Journal

JOURNAL OF THE AMERICAN CHEMICAL SOCIETY
Volume 133, Issue 13, Pages 4810-4818

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/ja108341t

Keywords

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Funding

  1. National Science Foundation [CHE-1012833, CHE-0840505]
  2. Division Of Chemistry
  3. Direct For Mathematical & Physical Scien [1012833] Funding Source: National Science Foundation

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Ensemble infrared photodissociation (IRFD) spectra in the hydrogen stretch region (similar to 2950-3800 cm(-1)) are reported for M(H2O)(35-37), with M = I-, Cl-, HCO3-, OH-, tetrabutyl-, tetrapropyl-, and tetramethylammonium, Cs+, Na+, Li+, H+, Ba2+, Ca2+, Co2+, Mg2+, La3+, and Tm3+, at 133 K. A single, broad feature is observed in the bonded-OH region of the spectra that indicates that the water network in these clusters is bulk-like and likely resembles liquid water more strongly than ice. The free-OH region for all of these clusters is dominated by peaks corresponding to water molecules that accept two and donate one hydrogen bond (AAD water molecules), indicating that AAD water molecules are more abundant at the surface of these. ions than AD water molecules. A-only water molecules are present in significant abundance only for the trivalent metal cations. The frequency of the AAD free-OH stretch band shifts nearly linearly with the charge state of the ion, consistent with a Stark shift attributable to the ion's electric field. From these data, a frequency range of 3704.9-3709.7 cm(-1) is extrapolated for the free-OH of AAD water molecules at the (uncharged) bulk liquid water surface, consistent with sum-frequency generation spectroscopy experiments. Differences in both the bonded- and the free-OH regions of the spectra for these ions are attributable to ion-induced patterning of the water network that extends to the surface of the clusters, which includes water molecules in the third and fourth solvation shells; that is, these ions pattern water molecules at long distance to various extents. These spectra are simulated using two different electrostatic models previously used to calculate OH-stretch spectra of bulk water and aqueous solutions and parametrized for bonded-OH frequencies. These models qualitatively reproduce a number of features in the experimental spectra, although it is evident that more sophisticated treatment of water molecule and ion polarizability and vibrational coupling is necessary for more quantitative comparisons.

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