2009
DOI: 10.1088/0022-3727/42/6/065107
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Sputter-deposited Mg–Al–O thin films: linking molecular dynamics simulations to experiments

Abstract: Using a molecular dynamics model the crystallinity of Mg x Al y O z thin films with a variation in the stoichiometry of the thin film is studied at operating conditions similar to the experimental operating conditions of a dual magnetron sputter deposition system. The films are deposited on a crystalline or amorphous substrate. The Mg metal content in the film ranged from 100% (i.e. MgO film) to 0% (i.e. Al 2 O 3 film). The radial distribution function and density of the films are calculated. The results are c… Show more

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Cited by 44 publications
(61 citation statements)
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“…The Cr 2 O 3 film is a mixture of polycrystalline and amorphous phases. Similar results were also obtained for Mg x Al y O z films and were confirmed by X-ray diffraction and transmission electron microscopy, as is explained in detail in [31]. The simulation time per impact in these MD simulations is 2-4 ps, followed by 2-6 ps of relaxation before the next impact takes place.…”
Section: Modeling the Plasma-surface Interactionssupporting
confidence: 84%
“…The Cr 2 O 3 film is a mixture of polycrystalline and amorphous phases. Similar results were also obtained for Mg x Al y O z films and were confirmed by X-ray diffraction and transmission electron microscopy, as is explained in detail in [31]. The simulation time per impact in these MD simulations is 2-4 ps, followed by 2-6 ps of relaxation before the next impact takes place.…”
Section: Modeling the Plasma-surface Interactionssupporting
confidence: 84%
“…21 This potential has been developed over many years and extensively applied to investigate the growth processes of Y 2 O 3 , ZrO 2 and MgAl-O thin films. [22][23][24][25][26] Here we show that high-κ bulk materials of amorphous nature can be generated quite efficiently using this particular potential function. Detailed analysis of the amorphous structures are carried out including the coordination number, the radial distribution function and the potential energy per atom of the structures.…”
Section: Introductionmentioning
confidence: 91%
“…[31] thermal activated diffusion during the time between arriving atoms is neglected. Another approach is to switch between NVE and NVT ensembles to make sure that the system relaxes after each deposition event [49]. Since the present model treats diffusion via Langevin dynamics, it is possible to preserve a realistic value for the mean squared displacement of neighborless particles during the time between two deposition events.…”
Section: A Details Of the Modelmentioning
confidence: 99%