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Structures and Spectroscopic Properties of F<sup>–</sup>(H<sub>2</sub>O)<sub><i>n</i></sub> with <i>n</i> = 1–10 Clusters from a Global Search Based On Density Functional Theory
17
Citations
71
References
2018
Year
Using a genetic algorithm incorporated in density functional theory, we explore the ground state structures of fluoride anion-water clusters F<sup>-</sup>(H<sub>2</sub>O) <sub>n</sub> with n = 1-10. The F<sup>-</sup>(H<sub>2</sub>O) <sub>n</sub> clusters prefer structures in which the F<sup>-</sup> anion remains at the surface of the structure and coordinates with four water molecules, as the F<sup>-</sup>(H<sub>2</sub>O) <sub>n</sub> clusters have strong F<sup>-</sup>-H<sub>2</sub>O interactions as well as strong hydrogen bonds between H<sub>2</sub>O molecules. The strong interaction between the F<sup>-</sup> anion and adjacent H<sub>2</sub>O molecule leads to a longer O-H distance in the adjacent molecule than in an individual water molecule. The simulated infrared (IR) spectra of the F<sup>-</sup>(H<sub>2</sub>O)<sub>1-5</sub> clusters obtained via second-order vibrational perturbation theory (VPT2) and including anharmonic effects reproduce the experimental results quite well. The strong interaction between the F<sup>-</sup> anion and water molecules results in a large redshift (600-2300 cm<sup>-1</sup>) of the adjacent O-H stretching mode. Natural bond orbital (NBO) analysis of the lowest-energy structures of the F<sup>-</sup>(H<sub>2</sub>O)<sub>1-10</sub> clusters illustrates that charge transfer from the lone pair electron orbital of F<sup>-</sup> to the antibonding orbital of the adjacent O-H is mainly responsible for the strong interaction between the F<sup>-</sup> anion and water molecules, which leads to distinctly different geometric and vibrational properties compared with neutral water clusters.
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