Electron spectroscopy study of hydrogenated amorphous carbon films formed by methane ion beam deposition

1984 ◽  
Vol 120 (3) ◽  
pp. 231-238 ◽  
Author(s):  
P. Oelhafen ◽  
J.L. Freeouf ◽  
J.M.E. Harper ◽  
J.J. Cuomo
1981 ◽  
Vol 7 ◽  
Author(s):  
John C. Angus ◽  
Michael J. Mirtich ◽  
Edwin G. Wintucky

ABSTRACTCarbon films were deposited on silicon, quartz, and potassium bromide substrates from an ion beam. Growth rates were approximately 0.3 μm/hour. The films were featureless and amorphous and contained only carbon and hydrogen in significant amounts. The density and carbon/hydrogen ratio indicate the film is a hydrogen deficient polymer. One possible structure, consistent with the data, is a random network of methylene linkages and tetrahedrally coordinated carbon atoms.


2000 ◽  
Vol 648 ◽  
Author(s):  
A.Yu. Belov ◽  
H.U. Jäger

AbstractAtomic-scale calculations were performed for the first time to investigate mechanical properties of amorphous carbon films grown by a realistic simulation of ion-beam deposition. The simulated films have a thickness of a few nanometers and reproduce the main structural features of real films, with the bulk content of sp3 bonded atoms varying from 35 to 95%, depending on the ion energy (E = 20-80 eV). Employing empirical interatomic potentials for carbon, the average bulk stresses as well as the atomic-level stress distributions were calculated and analysed. The bulk stresses were found to depend not only on the ion energy, but also on the film quality, in particular, on such structural inhomogeneities as local fluctuations of the sp3 fraction with the depth. The local variation of the bulk stress from the average value considerably increases as the local content of sp2 bonded atoms increases. Elastic constants of amorphous carbon films were also computed using the method of inner elastic constants, which allows for the stress dependence of elastic constants to be analysed. The variation of Young's modulus as a function of the lateral bulk stress in an amorphous film is demonstrated.


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