Neutral-atom scattering from random isolated adsorbate atoms on clean metal surfaces: Oxygen and carbon monoxide on nickel (001)

1983 ◽  
Vol 28 (6) ◽  
pp. 3164-3172 ◽  
Author(s):  
J. Ibáñez ◽  
N. García ◽  
J. M. Rojo
1977 ◽  
Vol 16 (3) ◽  
pp. 921-926 ◽  
Author(s):  
M. J. Mehl ◽  
W. L. Schaich

2D Materials ◽  
2018 ◽  
Vol 5 (4) ◽  
pp. 045002 ◽  
Author(s):  
Amjad Al Taleb ◽  
Gloria Anemone ◽  
Rodolfo Miranda ◽  
Daniel Farías
Keyword(s):  

1974 ◽  
Vol 29 (2) ◽  
pp. 189-193 ◽  
Author(s):  
George Comsa ◽  
Gerda H. Comsa ◽  
J. K. Fremerey

Some of the peculiarities of the atom scattering on metal surfaces are discussed in connection with the applicability of the Debye-Waller factor (DWF). The influence of the attractive potential well and of the finite size of the incident particles upon the scattering is commented. By comparing calculated DWF-values with experimental He scattering data it is concluded that the existence of diffraction is a necessary but not a sufficient condition for the applicability of the DWF. It is finally shown that the smooth potential surfaces which characterize the interaction between atoms and metal surfaces explain the apparently reduced thermal roughening observed experimentally.


The friction behaviour of iron and Fe-Cr alloys in unidirectional and reciprocating sliding motions at 293 K has been examined in oxygen of controlled partial pressure. During sliding, a progressive decrease in coefficient of friction accompanies the development of compacted oxide films on the metal surfaces, eventually resulting in a steady value of about 0.6 when almost complete oxide coverage is attained. This is achieved more rapidly at higher oxygen partial pressures. A model to account for the experimental observations is proposed, based on the growth of oxide on the clean metal surfaces and metal wear particles between each wear traversal and the removal of that oxide during the subsequent traversal. The oxidized debris is fragmented further and compacted on to the metal surfaces to form a layer of nominally constant thickness, the area of which increases progressively with the number of sliding traversals. The model relates the coefficient of friction to the area of compacted oxide in terms of several interfacial metal, oxide and metal-oxide parameters. The importance of some of these parameters on the frictional behaviour is discussed in light of the experimental observations.


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