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Spectroscopic observation of two-center three-electron bonded (hemi-bonded) structures of (H(2)S)(n) (+) clusters in the gas phase
A two-center three-electron 2c–3e bond (hemi-bond) is a non-classical chemical bond, and its existence has been supposed in radical cation clusters with lone pairs. Though the nature of the hemi-bond and its role in the reactivity of radical cations have attracted great interest, spectroscopic obser...
Autores principales: | , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Royal Society of Chemistry
2017
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5433515/ https://www.ncbi.nlm.nih.gov/pubmed/28553502 http://dx.doi.org/10.1039/c6sc05361k |
Sumario: | A two-center three-electron 2c–3e bond (hemi-bond) is a non-classical chemical bond, and its existence has been supposed in radical cation clusters with lone pairs. Though the nature of the hemi-bond and its role in the reactivity of radical cations have attracted great interest, spectroscopic observations of hemi-bonded structures have been very scarce. In the present study, the presence of a stable hemi-bonded core (H(2)S∴SH(2))(+) in (H(2)S)(n) (+) (n = 3–6) in the gas phase is demonstrated by infrared spectroscopy combined with quantum chemical calculations. The spectral features of the free SH stretch of the ion core show that the hemi-bond motif of the ion core is maintained up to the completion of the first H-bonded solvation shell. All of the observed spectra are well reproduced by the minimum energy hemi-bonded isomers, and no sign of the proton-transferred ion core type H(3)S(+)–SH, which is estimated to have a much higher energy, is found. Spin density calculations show that the excess charge is almost equally delocalized over the two H(2)S molecules in the cluster for n = 3 to 6. This also indicates the hemi-bond nature of the (H(2)S∴SH(2))(+) ion core and the small impact of the formation of a solvation shell on the ion core. |
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