Abstract

Laser-induced desorption of metal atoms at low rate has been studied for pulsed excitation with wavelengths of λ = 266, 355, 532 and 1064 nm. For this purpose sodium adsorbed on quartz served as a model system. The detached Na atoms were photo-ionized with the light of a second laser operating at λ = 193 nm and their kinetic energy distribution was determined by time-of-flight measurements. For λ = 1064 nm a distribution typical of thermal bond breaking is observed. If desorption, however, is stimulated with light of λ = 266 or 532 nm, the kinetic energy distribution is non-thermal with a single maximum atEkin = 0.16 ± 0.02 eV. For λ = 355 nm the non-thermal distribution is even bimodal with maxima appearing atEkin = 0.16 ± 0.02 and 0.33 ± 0.02 eV. These values of the kinetic energies actually remain constant under variation of all experimental parameters. They appear to reflect the electronic and geometric properties of different binding sites from which the atoms are detached and thus constitute fingerprints of the metal surface. The non-thermal desorption mechanism is discussed in the framework of the Menzel-Gomer-Redhead scenario. The transition from non-thermal to thermal desorption at large fluentes of the laser light could also be identified.

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