Molecular Dynamics Simulations of the Sputtering of β-SiC by Ar

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Molecular Dynamics Simulations of the Sputtering of β-SiC by Ar A.P. Prskalo; S. Schmauder; C. Kohler, IMWF, University of Stuttgart, Pfaffenwaldring 32, 70569 Stuttgart C. Ziebert, J. Ye, S. Ulrich, IMF I, Forschungszentrum Karlsruhe GmbH, Hermann-von-Helmholtz-Platz1, 76344 Eggenstein-Leopoldshafen Introduction Migration energy The overall research goal is to use molecular dynamics simulations in combination with experimental validation for the development of improved SiC and SiN single- and bilayer coatings, and multilayer SiC/SiN nanolaminates, which are deposited by magnetron sputtering onto silicon and/or steel. These materials are characterised by a high oxidation, wear and thermal resistance. As a first step for the development of SiC/SiN nanolaminates the sputtering of a SiC-target at 700 K by argon was simulated by the method of molecular dynamics using the Tersoff potential for the Si-C interaction and tabulated ZBL pair potential for the interaction with argon. Mobility of atoms and holes inside an SiC-crystal Distinction between two sublattices (Si and C) Potential barriers of different heights depending on the considered sublattice and the behaviour of surrounding atoms Thermal expansion and melting temperature of SiC Cubic SiC-target consisting of 4096 atoms heated from 0K to 5000K Npt-ensemble with external pressure (isotropic volume scaling) and temperature (Nose-Hoover thermostat) control Imposed temperature linearly varied over 108 time steps, each time step being 0.1 fs long Discontinuity in the temperature regime indicates phase transition Coefficient of thermal expansion of β-SiC is α=1.1·10-5 and the melting temperature is 3920 K Sputtering of beta-SiC by Ar Monocrystal of β-SiC in the dimensions of 10·10·20 unit cells Equilibriation of the target material at 700K using npt-simulation as described. Usage of 50 thermic equivalent probes to achieve statistics Surface binding energy For sputtering, the kinetic energy of the surface atoms must exceed the surface binding energy. Distinction between four surface binding energies, two types of surfaces, with and without surface recombination Impact energies of the argon ion between 50 eV and 1 keV Distinction between C-surface and Si-surface terminated single crystal Analysis of different data types, in particular the penetration depth, front- and back sputtered atoms (sputter yield) Automatisation due to large amount of data This work was supported by the German Research Foundation DFG in the Project SCHM 746/68-1/ZI 1174/3-1 Contact: Dipl.-Phys. Alen-Pilip Prskalo Institut für Materialprüfung, Werkstoffkunde und Festigkeitslehre; Universität Stuttgart Pfaffenwaldring 32; 70569 Stuttgart Phone: +49 (0) 711 685-62579; E-Mail: alen-pilip.prskalo@mpa.uni-stuttgart.de