1551. Energy distribution of light ions scattered by solid surfaces

Vacuum ◽  
1968 ◽  
Vol 18 (12) ◽  
pp. 694
1983 ◽  
Vol 29 ◽  
Author(s):  
J. Hager ◽  
H. Walther

ABSTRACTThe internal energy distribution of NO molecules scattered from different solid surfaces (Pt(111), graphite, and Pt(111) covered with various adlayers) was investigated by the laser-induced fluorescence method. In the case of the NO/graphite system, moreover, the velocity distribution of the scattered molecules could be measured in a time-offlight experiment. The rotational energy distribution, which can always be described as a Boltzmann distribution, exhibits only partial accommodation to the surface temperature for all surfaces investigated. The measurements of the velocity of the NO molecules scattered from the graphite surface show only a small influence of the surface temperature on the average velocity and on the velocity distribution. Furthermore, the measured velocity distribution is independent of the final rotational state of the scattered molecules. On the basis of these results, a rather complete description of the behavior of the NO molecules during the scattering process can be presented.


1972 ◽  
Vol 13 (1-2) ◽  
pp. 131-135 ◽  
Author(s):  
E. S. Mashkova ◽  
V. A. Molchanov

1992 ◽  
Vol 69 (2-3) ◽  
pp. 429-438 ◽  
Author(s):  
A.A. Sonzogni ◽  
A.S.M.A. Romo ◽  
W.R. Frosch ◽  
S.J. Nassiff

1973 ◽  
Vol 20 (1-2) ◽  
pp. 65-67 ◽  
Author(s):  
J. B⊘ttiger ◽  
K. B. Winterbon

1999 ◽  
Vol 60 (9) ◽  
pp. 6352-6356 ◽  
Author(s):  
G. Falcone ◽  
L. Forlano ◽  
A. I. Tolmachev

The distributions in angle an d energy for charged particles emitted from polycrystalline and crystalline platinum (100 face) bombarded with ions of hydrogen, nitrogen and argon, have been m easured, in continuation of previous work (Cawthron, Cotterell & Oliphant 1969, part I and II). Hydrogenions incident on polycrystalline platinum , with energy of the order of 10 keV, give distributions with angle of incidence, α, and angle of scattering, θ, in general accord with what might be expected, but the heavier ions show marked differences, probably due to some sputtered atom s escaping with electric charge. With the crystalline target, where effects of channelling were observed in the angular distribution of emitted charged particles, these were accompanied by marked changes in the energy distribution of these scattered particles.


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