TY - JOUR
T1 - Resonant IR laser stimulation of the desorption of methanol adsorbed on Cu(110)
AU - Peremans, André
AU - Dereux, Alain
AU - Maseri, Fabrizio
AU - Darville, Jacques
AU - Gilles, Jean-Marie
AU - Vigneron, Jean-Pol
PY - 1992
Y1 - 1992
N2 - The reactive system CH3OH/Cu(110) has been characterized by thermal desorption and infrared reflection-absorption spectroscopies. This provides the knowledge of the reactive system properties necessary for the interpretation of the ir photodesorption experimental results. These properties are the sticking coefficient of methanol on Cu(110) at 90 K, the monolayer density, the ir absorbance, and the structure of the adsorbate. In particular, ir spectroscopy demonstrates the possibility of thermally activating the crystallization of the amorphous adsorbate obtained upon condensation on Cu(110) at 90 K. The experimental setup used for the measurements of the photodesorption yield (YPD) makes use of an optical parametric oscillator generating ir pulses about 15 ns long and frequencies tunable from 2800 to 3450 cm.−1 This frequency range includes the ir bands corresponding to the asymmetric methyl and hydroxyl stretching modes. The ir YPD of amorphous and crystallized films have been measured as a function of the laser-beam frequency and fluence, of the substrate coverage, and of the temperature (from 90 to 120 K). The correspondence between the YPD spectra and the ir spectrum of liquid methanol indicates the occurrence of adsorbate melting during the photodesorption process. The saturable exponential evolution of the YPD as a function of the laser fluence reveals the thermal nature of the process. The YPD of the amorphous methanol thin films increases greatly upon their crystallization. This is tentatively explained as a consequence of a change in the film morphology. These experimental results are interpreted quantitatively in the framework of the thermal photodesorption mechanism due to the resonant substrate heating.
AB - The reactive system CH3OH/Cu(110) has been characterized by thermal desorption and infrared reflection-absorption spectroscopies. This provides the knowledge of the reactive system properties necessary for the interpretation of the ir photodesorption experimental results. These properties are the sticking coefficient of methanol on Cu(110) at 90 K, the monolayer density, the ir absorbance, and the structure of the adsorbate. In particular, ir spectroscopy demonstrates the possibility of thermally activating the crystallization of the amorphous adsorbate obtained upon condensation on Cu(110) at 90 K. The experimental setup used for the measurements of the photodesorption yield (YPD) makes use of an optical parametric oscillator generating ir pulses about 15 ns long and frequencies tunable from 2800 to 3450 cm.−1 This frequency range includes the ir bands corresponding to the asymmetric methyl and hydroxyl stretching modes. The ir YPD of amorphous and crystallized films have been measured as a function of the laser-beam frequency and fluence, of the substrate coverage, and of the temperature (from 90 to 120 K). The correspondence between the YPD spectra and the ir spectrum of liquid methanol indicates the occurrence of adsorbate melting during the photodesorption process. The saturable exponential evolution of the YPD as a function of the laser fluence reveals the thermal nature of the process. The YPD of the amorphous methanol thin films increases greatly upon their crystallization. This is tentatively explained as a consequence of a change in the film morphology. These experimental results are interpreted quantitatively in the framework of the thermal photodesorption mechanism due to the resonant substrate heating.
U2 - 10.1103/PhysRevB.45.8598
DO - 10.1103/PhysRevB.45.8598
M3 - Article
SN - 0163-1829
VL - 45
SP - 8598
EP - 8609
JO - Physical review. B, Condensed matter
JF - Physical review. B, Condensed matter
IS - 15
ER -