TY - JOUR
T1 - The first layer of water on Rh(111)
T2 - Microscopic structure and desorption kinetics
AU - Beniya, Atsushi
AU - Yamamoto, Susumu
AU - Mukai, Kozo
AU - Yamashita, Yoshiyuki
AU - Yoshinobu, Jun
N1 - Funding Information:
Financial support was provided in part by the Grant-in-Aid for Scientific Research on Priority Areas “Surface Chemistry of Condensed Molecules” from the Ministry of Education, Culture, Sports, Science and Technology (MEXT) of Japan. One of the authors (A.B.) is supported by the program “The 21st century COE program for Applied Physics on Strong Correlation” at the University of Tokyo.
PY - 2006
Y1 - 2006
N2 - The adsorption states and growth process of the first water (D 2O) layer on Rh(111) were investigated using infrared reflection absorption spectroscopy, temperature programed desorption, and spot-profile-analysis low energy electron diffraction. Water molecules wet the Rh(111) surface intact. At the early stage of first layer growth, a (√3 × √3)R30ο commensurate water layer grows where "up" and "down" species coexist; the up and down species represent water molecules which have free OD, pointing to a vacuum and the substrate, respectively. The up domain was a flatter structure than an icelike bilayer. Water desorption from Rh(111) was a half-order process. The activation energy and the preexponential factor of desorption are estimated to be 60 kJ/ mol and 4.8 × 10 16 ML 1/2/s at submonolayer coverage, respectively. With an increase in water coverage, the flat up domain becomes a zigzag layer, like an ice bilayer. At the saturation coverage, the amount of down species is 1.3 times larger than that of the up species. In addition, the activation energy and the preexponential factor of desorption decrease to 51 kJ/mol and 1.3 × 10 14 ML 1/2/s, respectively.
AB - The adsorption states and growth process of the first water (D 2O) layer on Rh(111) were investigated using infrared reflection absorption spectroscopy, temperature programed desorption, and spot-profile-analysis low energy electron diffraction. Water molecules wet the Rh(111) surface intact. At the early stage of first layer growth, a (√3 × √3)R30ο commensurate water layer grows where "up" and "down" species coexist; the up and down species represent water molecules which have free OD, pointing to a vacuum and the substrate, respectively. The up domain was a flatter structure than an icelike bilayer. Water desorption from Rh(111) was a half-order process. The activation energy and the preexponential factor of desorption are estimated to be 60 kJ/ mol and 4.8 × 10 16 ML 1/2/s at submonolayer coverage, respectively. With an increase in water coverage, the flat up domain becomes a zigzag layer, like an ice bilayer. At the saturation coverage, the amount of down species is 1.3 times larger than that of the up species. In addition, the activation energy and the preexponential factor of desorption decrease to 51 kJ/mol and 1.3 × 10 14 ML 1/2/s, respectively.
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U2 - 10.1063/1.2227393
DO - 10.1063/1.2227393
M3 - Article
AN - SCOPUS:33746924098
SN - 0021-9606
VL - 125
JO - Journal of Chemical Physics
JF - Journal of Chemical Physics
IS - 5
M1 - 054717
ER -