The Influence of Clusters on Vapor-Deposited thin Films: Atomistic Simulations

2000 ◽  
Vol 616 ◽  
Author(s):  
J. Dalla Torreg ◽  
G. H. Gilmer ◽  
F. H. Baumann ◽  
P. O'Sullivan ◽  
M. Djafari Rouhani

AbstractWe investigate the morphology of films produced by cluster deposition using Monte Carlo atomistic simulations. Thin films of aluminum are considered as an example. The deposition of small Al clusters containing up to 5 atoms is simulated. Compared with monomer beams, Al cluster deposition increases the density of 3D islands nucleated on the substrate and tends to equalize the growth rate of the different crystal facets. We discuss the smoothening of the surface when the 3D islands merge. We find that there is an optimal size of the deposited clusters that produces the smoothest film.

2019 ◽  
Vol 21 (19) ◽  
pp. 9802-9809
Author(s):  
John A. Purton

The mobility of oxygen ions at surfaces and interfaces in solid oxide fuel materials are examined using atomistic simulations.


Author(s):  
D. R. Liu ◽  
S. S. Shinozaki ◽  
R. J. Baird

The epitaxially grown (GaAs)Ge thin film has been arousing much interest because it is one of metastable alloys of III-V compound semiconductors with germanium and a possible candidate in optoelectronic applications. It is important to be able to accurately determine the composition of the film, particularly whether or not the GaAs component is in stoichiometry, but x-ray energy dispersive analysis (EDS) cannot meet this need. The thickness of the film is usually about 0.5-1.5 μm. If Kα peaks are used for quantification, the accelerating voltage must be more than 10 kV in order for these peaks to be excited. Under this voltage, the generation depth of x-ray photons approaches 1 μm, as evidenced by a Monte Carlo simulation and actual x-ray intensity measurement as discussed below. If a lower voltage is used to reduce the generation depth, their L peaks have to be used. But these L peaks actually are merged as one big hump simply because the atomic numbers of these three elements are relatively small and close together, and the EDS energy resolution is limited.


1994 ◽  
Vol 4 (7) ◽  
pp. 991-995 ◽  
Author(s):  
J. F. Roux ◽  
M. Treilleux ◽  
B. Cabaud ◽  
G. Fuchs ◽  
C. Montandon ◽  
...  

2007 ◽  
Vol 992 ◽  
Author(s):  
Christos F. Karanikas ◽  
James J. Watkins

AbstractThe kinetics of the deposition of ruthenium thin films from the hydrogen assisted reduction of bis(2,2,6,6-tetramethyl-3,5-heptanedionato)(1,5-cyclooctadiene)ruthenium(II), [Ru(tmhd)2cod], in supercritical carbon dioxide was studied in order to develop a rate expression for the growth rate as well as to determine a mechanism for the process. The deposition temperature was varied from 240°C to 280°C and the apparent activation energy was 45.3 kJ/mol. Deposition rates up to 30 nm/min were attained. The deposition rate dependence on precursor concentrations between 0 and 0.2 wt. % was studied at 260°C with excess hydrogen and revealed first order deposition kinetics with respect to precursor at concentrations lower then 0.06 wt. % and zero order dependence at concentrations above 0.06 wt. %. The effect of reaction pressure on the growth rate was studied at a constant reaction temperature of 260°C and pressures between 159 bar to 200 bar and found to have no measurable effect on the growth rate.


1977 ◽  
Vol 40 (1) ◽  
pp. 47-58 ◽  
Author(s):  
D. Kashchiev ◽  
J.P. van der Eerden ◽  
C. van Leeuwen

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