TY - JOUR
T1 - Resonant photodissociation of Mo(CO)6 adsorbed on graphite and Ag(111)
AU - So, S. K.
AU - Ho, W.
N1 - Funding information:
Support of this research by the Office of Naval Research under Grant No. NOOO14-90-J-1214 and the Cornell Materials Science Center through the National Science Foundation, Grant No. DMR-88-18558, is gratefully acknowledged. We would like to thank Dr. D. V. Chakarov, Walter Mieher, and Dr. Z. C. Ying for stimulating discussions and a critical reading of the manuscript, and Bengt Kasemo and Peter Sj6vall for providing us with the graphite sample.
Publisher copyright:
© 1991 American Institute of Physics
PY - 1991/7/1
Y1 - 1991/7/1
N2 - The adsorption and photodissociation of Mo(CO)6 on the basal plane of graphite and Ag (111) are studied by photoinduced desorption, high-resolution electron-energy-loss spectroscopy, electronic electron-energy-loss spectroscopy (EELS), and thermal desorption spectroscopy. Mo(CO)6 is found to absorb in pure molecular form, without dissociation, on each surface at 85-90 K. Electronic EEL spectra confirm that the electronic structure of the molecule remains relatively unperturbed on the surface. Similar to the gas phase, electronic transitions of the molecule, including the ligand-field transition and the metal-to-ligand charge transfer, were observed for absorbed Mo(CO)6. Upon low-power UV irradiation (λ < 360 nm), the adsorbed molecules readily photodissociate and release CO. The mechanism of photodissociation on each surface is separately identified to be direct photoelectronic excitation of the adsorbed Mo(CO) 6 by careful photon power and wavelength-dependence studies. Linear power dependence was found in each case, indicating the initial excitation is due to the absorption of a single photon. Resonances in the photodissociation spectra of the molecules were observed at ∼290 nm and 325 nm, due to the metal-to-ligand charge transfer and the ligand-field transition, respectively. For graphite, the relative photoyield was observed to closely match the Mo(CO)6 absorption spectrum. In contrast, a relative enhancement in the photoyield was observed for Ag(111) at ∼325 nm due to the increase of the surface electric field associated with the onset of the d band to the Fermi-level transition in this wavelength region. In addition, small quantities of the fragments from Mo(CO)6 were observed as a result of bombardment of the surface by low-energy (20 eV) electrons. The photodissociation yields are very sensitive to the adsorbate coverage. For a coverage of about 0.25 monolayer or less, there is no observable photodissociation for Mo(CO)6 on Ag. On both Ag and graphite, the photodissociation yield increases as the coverage approaches and exceeds one monolayer; photodissociation competes efficiently with relaxation into the substrate.
AB - The adsorption and photodissociation of Mo(CO)6 on the basal plane of graphite and Ag (111) are studied by photoinduced desorption, high-resolution electron-energy-loss spectroscopy, electronic electron-energy-loss spectroscopy (EELS), and thermal desorption spectroscopy. Mo(CO)6 is found to absorb in pure molecular form, without dissociation, on each surface at 85-90 K. Electronic EEL spectra confirm that the electronic structure of the molecule remains relatively unperturbed on the surface. Similar to the gas phase, electronic transitions of the molecule, including the ligand-field transition and the metal-to-ligand charge transfer, were observed for absorbed Mo(CO)6. Upon low-power UV irradiation (λ < 360 nm), the adsorbed molecules readily photodissociate and release CO. The mechanism of photodissociation on each surface is separately identified to be direct photoelectronic excitation of the adsorbed Mo(CO) 6 by careful photon power and wavelength-dependence studies. Linear power dependence was found in each case, indicating the initial excitation is due to the absorption of a single photon. Resonances in the photodissociation spectra of the molecules were observed at ∼290 nm and 325 nm, due to the metal-to-ligand charge transfer and the ligand-field transition, respectively. For graphite, the relative photoyield was observed to closely match the Mo(CO)6 absorption spectrum. In contrast, a relative enhancement in the photoyield was observed for Ag(111) at ∼325 nm due to the increase of the surface electric field associated with the onset of the d band to the Fermi-level transition in this wavelength region. In addition, small quantities of the fragments from Mo(CO)6 were observed as a result of bombardment of the surface by low-energy (20 eV) electrons. The photodissociation yields are very sensitive to the adsorbate coverage. For a coverage of about 0.25 monolayer or less, there is no observable photodissociation for Mo(CO)6 on Ag. On both Ag and graphite, the photodissociation yield increases as the coverage approaches and exceeds one monolayer; photodissociation competes efficiently with relaxation into the substrate.
UR - http://www.scopus.com/inward/record.url?scp=0000161632&partnerID=8YFLogxK
U2 - 10.1063/1.461416
DO - 10.1063/1.461416
M3 - Journal article
AN - SCOPUS:0000161632
SN - 0021-9606
VL - 95
SP - 656
EP - 671
JO - The Journal of Chemical Physics
JF - The Journal of Chemical Physics
IS - 1
ER -