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Revisit the landscape of protonated water clusters H+(H2O)n with <i>n</i> = 10–17: An <i>ab initio</i> global search

17

Citations

61

References

2018

Year

Abstract

Using a genetic algorithm incorporated with density functional theory, we explore the ground state structures of protonated water clusters H<sup>+</sup>(H<sub>2</sub>O)<sub>n</sub> with n = 10-17. Then we re-optimize the isomers at B97-D/aug-cc-pVDZ level of theory. The extra proton connects with a H<sub>2</sub>O molecule to form a H<sub>3</sub>O<sup>+</sup> ion in all H<sup>+</sup>(H<sub>2</sub>O)<sub>10-17</sub> clusters. The lowest-energy structures adopt a monocage form at n = 10-16 and core-shell structure at n = 17 based on the MP2/aug-cc-pVTZ//B97-D/aug-cc-pVDZ+ZPE single-point-energy calculation. Using second-order vibrational perturbation theory, we further calculate the infrared spectra with anharmonic correction for the ground state structures of H<sup>+</sup>(H<sub>2</sub>O)<sub>10-17</sub> clusters at the PBE0/aug-cc-pVDZ level. The anharmonic correction to the spectra is crucial since it reproduces the experimental results quite well. The extra proton weakens the O-H bond strength in the H<sub>3</sub>O<sup>+</sup> ion since the Wiberg bond order of the O-H bond in the H<sub>3</sub>O<sup>+</sup> ion is smaller than that in H<sub>2</sub>O molecules, which causes a red shift of the O-H stretching mode in the H<sub>3</sub>O<sup>+</sup> ion.

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