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Molecular dynamics simulations of the initial stages of sputter erosion of a metal overlayer system: 2 keV Ar → Cu/Ni(1 0 0)

✍ Scribed by M.A. Karolewski


Publisher
Elsevier Science
Year
2006
Tongue
English
Weight
758 KB
Volume
243
Category
Article
ISSN
0168-583X

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✦ Synopsis


The initial sputter erosion of Cu/Ni(1 0 0) has been simulated using molecular dynamics. The morphological and compositional changes that accompany sputtering are described. Ar projectiles (2 keV) are delivered sequentially at 10 ps intervals into a 2000 A ˚2 region of the target, up to a nominal fluence of 1.1 • 10 15 cm À2 . Simulations were performed for several projectile-target geometries with normal, oblique and random altitudinal (u) angles of incidence and h0 1 1i, h0 0 1i and random azimuthal (/) angles of incidence. As expected, the predicted rate of target erosion is lowest for normal projectile incidence, and increases for oblique bombardment geometries. The predicted sputtering properties show no significant dependence on / (for u = 70°). The principal effect of bombardment geometry is to alter the rate at which surface erosion proceeds. However, differences in the morphological development of the target are detected for the oblique bombardment geometry with u = 30°(e.g. a reduction in the sputtered atom information depth). This geometry also causes a displacement (by 20 A ˚) of the sputtering crater from the centre of the primary impact zone. With reference to observations made on an experimental timescale, the simulations are deficient in terms of their ability to model diffusive processes, e.g. the annihilation of adatom monomers on terraces outside the primary impact zone.


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Molecular dynamics of thermal vibration
✍ Yakup Hundur; Ziya B. Güvenç; Rainer Hippler 📂 Article 📅 2010 🏛 Elsevier Science 🌐 English ⚖ 610 KB

In this work constant energy molecular dynamics simulations are achieved for investigating sputtering process of Ar + Ni(1 0 0) collision system. The Ni crystal is imitated by an embedded-atom potential, whereas the interaction between the projectile and the surface is modeled by re-parameterized ZB