TY - JOUR
T1 - Screening of SFG signals from bridged CO on Ni(111) by the coexistence of linear CO
AU - Katano, S.
AU - Bandara, A.
AU - Kubota, J.
AU - Onda, K.
AU - Wada, A.
AU - Domen, K.
AU - Hirose, C.
N1 - Funding Information:
The authors are indebted to Professor S.S. Kano of Hosei University for his valuable discussions. This work was supported by the Grant-in-Aids for Scientific Research from the Ministry of Education Science and Culture, Japan (Nos 06239110 and 08404039).
PY - 1999/6/1
Y1 - 1999/6/1
N2 - A spectroscopic study of adsorbed CO on Ni(111) was carried out using infrared-visible sum-frequency generation (SFG) and infrared reflection absorption spectroscopy (IRAS). An anomalous coverage-dependence of the SFG signal intensities of bridged and linear CO was found. While the SFG signal of bridged CO at 1920 cm-1 gained intensity with increasing CO coverage in the region between 0 and 0.4 ML (1 monolayer, ML: saturation coverage at 130 K), it weakened and disappeared when linear CO (2074 cm-1) was present on the surface above 0.47 ML. The IRA peak of bridged CO, however, did not disappear at the increased coverage suggesting that the weakening of the SFG signal of bridged CO is not caused by the decrease in the coverage but by the suppression of the SFG process of bridged CO by the coexistence of linear CO. The spectra of isotope mixtures of C16O and C18O clearly indicated that the weakening of SFG signals is not caused by the dipole-dipole coupling between the vibrational modes of bridged and linear CO. The anomalous coverage-dependence of the SFG signal was ascribed to the change of the Raman tensor by the coadsorption of linear CO.
AB - A spectroscopic study of adsorbed CO on Ni(111) was carried out using infrared-visible sum-frequency generation (SFG) and infrared reflection absorption spectroscopy (IRAS). An anomalous coverage-dependence of the SFG signal intensities of bridged and linear CO was found. While the SFG signal of bridged CO at 1920 cm-1 gained intensity with increasing CO coverage in the region between 0 and 0.4 ML (1 monolayer, ML: saturation coverage at 130 K), it weakened and disappeared when linear CO (2074 cm-1) was present on the surface above 0.47 ML. The IRA peak of bridged CO, however, did not disappear at the increased coverage suggesting that the weakening of the SFG signal of bridged CO is not caused by the decrease in the coverage but by the suppression of the SFG process of bridged CO by the coexistence of linear CO. The spectra of isotope mixtures of C16O and C18O clearly indicated that the weakening of SFG signals is not caused by the dipole-dipole coupling between the vibrational modes of bridged and linear CO. The anomalous coverage-dependence of the SFG signal was ascribed to the change of the Raman tensor by the coadsorption of linear CO.
UR - http://www.scopus.com/inward/record.url?scp=0033149522&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0033149522&partnerID=8YFLogxK
U2 - 10.1016/S0039-6028(99)00299-X
DO - 10.1016/S0039-6028(99)00299-X
M3 - Conference article
AN - SCOPUS:0033149522
SN - 0039-6028
VL - 427-428
SP - 337
EP - 342
JO - Surface Science
JF - Surface Science
T2 - Proceedings of the 1998 9th International Conference on Vibrations at Surfaces (VAS9)
Y2 - 12 October 1998 through 16 October 1998
ER -