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Notes: We report molecular dynamics calculations and molecular beam experiments on trapping and desorption as a function of surface temperature and initial gas conditions for the Ar–Pt(111) system. The trapping process involves very rapid equilibration of the normal component of incidence velocity but extremely slow accommodation of the parallel component. At high surface temperatures for which the residence time of Ar is sufficiently short (e.g., roughly 40 ps at 273 K), trapped atoms desorb before their incident parallel velocity is thermalized. Thus trapping in the usual sense of complete equilibration with the surface does not occur; instead these quasitrapped atoms are characterized by full accommodation of only the normal velocity component. In both simulations and experiments there is a range of temperatures for which the desorbing flux associated with quasitrapping is distinguishable from the flux due to direct inelastic scattering. These results are qualitatively reproduced by a simple model for the time-varying velocity distribution of quasitrapped atoms, which treats the different components of velocity independently.

Notes: Magnetic imaging has been demonstrated by photoemission microscopy in which spatial resolution is achieved by scanning an aperture across the sample. To achieve magnetic contrast, the difference between photoemission current with right and left circularly polarized light is recorded while holding the aperture-surface distance to 30 nm. We used conical gold tips with apertures as small as 30 nm, drilled by a focused ion beam. Images of Co/Pt multilayer films show a magnetic contrast of ±2% and a resolution (25%–75% of a step) of 30 nm. Resolution better than 10 nm should be achievable with smaller apertures. With this imaging method, there is no magnetic interaction between sample and tip, and ultrafast time resolution should be achievable. © 2000 American Institute of Physics.

Notes: Studies of the reaction of H atoms with Cl chemisorbed on Au(111) reveal two dynamically distinct mechanisms. Some reactions occur on essentially a single gas-surface collision, by way of a so-called Eley–Rideal (ER) mechanism. Others occur between accommodated H and Cl atoms, by way of a so-called Langmuir–Hinschelwood (LH) mechanism. The dynamics of these processes has been characterized by combining molecular beam techniques with quantum-state-specific detection. Specifically, I have used molecular beam time-of-flight (TOF) techniques to determine angular and velocity distributions of the HCl product, and I have used resonance-enhanced multiphoton ionization to determine rotational and vibrational state distributions. The TOF and angular distributions provide clear evidence for the ER mechanism. This mechanism yields a fast (early) peak in the TOF distributions and a narrow angular distribution that is asymmetric with respect to the surface normal. Moreover, the peak in the angular distribution moves further away from the normal in the direction of the specular angle as the energy of the incident H atom is increased from 0.07 to 0.3 eV.The mean energy of the ER product is about 0.6 eV, but increases slightly with increasing incidence energy. In contrast, the LH mechanism yields a relatively slow (late) TOF component that approximately follows a Boltzmann distribution at the surface temperature (Ts) and disappears at Ts〈170 K. The form of the angular distribution of this LH component is close to a cosine function. The fast (ER) TOF component is itself found to be composed of at least two contributions, assigned to HCl product formed in v=0 and v=1 (with some contribution from v=2). The rotational state distribution for the HCl(v=0) product of the ER mechanism is found to be distinctly non-Boltzmann, with a mean rotational energy of about 0.11 eV, or about 5% of the available energy. The rotational distributions obtained for v=1 and v=2 are similar to those for v=0. The relatively small fraction of energy channelled into rotation is a consequence of the low H-atom mass. In contrast, the rotational distributions for HCl(v=0) due to the LH mechanism are consistent with Boltzmann distributions at Ts. The vibrational state distribution for the ER process peaks in v=1. The form of this distribution varies slightly with Ts, with about 30% in v=0, 55% in v=1, and 15% in v=2 states at Ts=600 K. The mean vibrational energy for the ER component is thus about 0.32 eV, or ∼14% of the available energy. This vibrational distribution is inconsistent with a simple attractive potential energy surface, which would lead to higher vibrational excitation. Either a large fraction of the energy is released as repulsion between the HCl and the surface, or vibrational energy is quenched, possibly by coupling between the departing molecule and the surface. The mean total energy carried away in the HCl product is only about half of that theoretically available. The total yield of the ER reaction increases rapidly with Ts, reaching a cross section of about 2×10−16 cm2 per Cl atom at Ts=600 K.