TY - JOUR
T1 - Infrared spectroscopy of Cu+ (H2 O)n and Ag+ (H2 O)n
T2 - Coordination and solvation of noble-metal ions
AU - Iino, Takuro
AU - Ohashi, Kazuhiko
AU - Inoue, Kazuya
AU - Judai, Ken
AU - Nishi, Nobuyuki
AU - Sekiya, Hiroshi
N1 - Funding Information:
The authors are grateful to Professor Y. Inokuchi for his help in the initial stage of the experiments on . The authors acknowledge Professor Duncan for the use of unpublished results from his group. This work was supported in part by the Joint Studies Program (2005) of the Institute for Molecular Science and by “Nanotechnology Support Project” and Grant-in-Aid for Scientific Research (No. 17550014) of the Ministry of Education, Culture, Sports, Science, and Technology (MEXT), Japan.
PY - 2007
Y1 - 2007
N2 - M+ (H2 O)n and M+ (H2 O)n Ar ions (M=Cu and Ag) are studied for exploring coordination and solvation structures of noble-metal ions. These species are produced in a laser-vaporization cluster source and probed with infrared (IR) photodissociation spectroscopy in the OH-stretch region using a triple quadrupole mass spectrometer. Density functional theory calculations are also carried out for analyzing the experimental IR spectra. Partially resolved rotational structure observed in the spectrum of Ag+ (H2 O)1 Ar indicates that the complex is quasilinear in an Ar- Ag+ -O configuration with the H atoms symmetrically displaced off axis. The spectra of the Ar-tagged M+ (H2 O)2 are consistent with twofold coordination with a linear O- M+ -O arrangement for these ions, which is stabilized by the s-d hybridization in M+. Hydrogen bonding between H2 O molecules is absent in Ag+ (H2 O)3 Ar but detected in Cu+ (H2 O)3 Ar through characteristic changes in the position and intensity of the OH-stretch transitions. The third H2 O attaches directly to Ag+ in a tricoordinated form, while it occupies a hydrogen-bonding site in the second shell of the dicoordinated Cu+. The preference of the tricoordination is attributable to the inefficient 5s-4d hybridization in Ag+, in contrast to the extensive 4s-3d hybridization in Cu+ which retains the dicoordination. This is most likely because the s-d energy gap of Ag+ is much larger than that of Cu+. The fourth H2 O occupies the second shells of the tricoordinated Ag+ and the dicoordinated Cu+, as extensive hydrogen bonding is observed in M+ (H2 O)4 Ar. Interestingly, the Ag+ (H2 O)4 Ar ions adopt not only the tricoordinated form but also the dicoordinated forms, which are absent in Ag+ (H2 O)3 Ar but revived at n=4. Size dependent variations in the spectra of Cu+ (H2 O)n for n=5-7 provide evidence for the completion of the second shell at n=6, where the dicoordinated Cu+ (H2 O)2 subunit is surrounded by four H2 O molecules. The gas-phase coordination number of Cu+ is 2 and the resulting linearly coordinated structure acts as the core of further solvation processes.
AB - M+ (H2 O)n and M+ (H2 O)n Ar ions (M=Cu and Ag) are studied for exploring coordination and solvation structures of noble-metal ions. These species are produced in a laser-vaporization cluster source and probed with infrared (IR) photodissociation spectroscopy in the OH-stretch region using a triple quadrupole mass spectrometer. Density functional theory calculations are also carried out for analyzing the experimental IR spectra. Partially resolved rotational structure observed in the spectrum of Ag+ (H2 O)1 Ar indicates that the complex is quasilinear in an Ar- Ag+ -O configuration with the H atoms symmetrically displaced off axis. The spectra of the Ar-tagged M+ (H2 O)2 are consistent with twofold coordination with a linear O- M+ -O arrangement for these ions, which is stabilized by the s-d hybridization in M+. Hydrogen bonding between H2 O molecules is absent in Ag+ (H2 O)3 Ar but detected in Cu+ (H2 O)3 Ar through characteristic changes in the position and intensity of the OH-stretch transitions. The third H2 O attaches directly to Ag+ in a tricoordinated form, while it occupies a hydrogen-bonding site in the second shell of the dicoordinated Cu+. The preference of the tricoordination is attributable to the inefficient 5s-4d hybridization in Ag+, in contrast to the extensive 4s-3d hybridization in Cu+ which retains the dicoordination. This is most likely because the s-d energy gap of Ag+ is much larger than that of Cu+. The fourth H2 O occupies the second shells of the tricoordinated Ag+ and the dicoordinated Cu+, as extensive hydrogen bonding is observed in M+ (H2 O)4 Ar. Interestingly, the Ag+ (H2 O)4 Ar ions adopt not only the tricoordinated form but also the dicoordinated forms, which are absent in Ag+ (H2 O)3 Ar but revived at n=4. Size dependent variations in the spectra of Cu+ (H2 O)n for n=5-7 provide evidence for the completion of the second shell at n=6, where the dicoordinated Cu+ (H2 O)2 subunit is surrounded by four H2 O molecules. The gas-phase coordination number of Cu+ is 2 and the resulting linearly coordinated structure acts as the core of further solvation processes.
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U2 - 10.1063/1.2730830
DO - 10.1063/1.2730830
M3 - Article
C2 - 17523799
AN - SCOPUS:34249039615
SN - 0021-9606
VL - 126
JO - Journal of Chemical Physics
JF - Journal of Chemical Physics
IS - 19
M1 - 194302
ER -