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NEEP 541 Molecular Dynamics

NEEP 541 Molecular Dynamics. Fall 2002 Jake Blanchard. Outline. Molecular Dynamics The Kalypso code Documentation Limitations Potentials Binding energy Temperature Electronic stopping. Molecular Dynamics. Codes Moldy Kalypso Mdrange Marlowe I’ll discuss choices made by Kalypso

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NEEP 541 Molecular Dynamics

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  1. NEEP 541Molecular Dynamics Fall 2002 Jake Blanchard

  2. Outline • Molecular Dynamics • The Kalypso code • Documentation • Limitations • Potentials • Binding energy • Temperature • Electronic stopping

  3. Molecular Dynamics • Codes • Moldy • Kalypso • Mdrange • Marlowe • I’ll discuss choices made by Kalypso • Other codes would make other choices

  4. Kalypso • Do not trust what comes out of kalypso, or any other code, without being aware of exactly what it is doing • It contains many assumptions and approximations that might not be valid for your situation • For many cases, scaling and relative changes are more valid than absolute values of results

  5. Kalypso • For studying atomic collisions in metals • Best-suited for single particle collisions with target atoms (sputtering, reflection, adsorption, implantation) • Could also model diffusion, defect stability, etc. • Cannot model semiconductors • Uses molecular dynamics • Potentials (many-body) are Sutton-Chen or “Tight-Binding”

  6. Codes • Spider is for preparing input files • Kalypso is for running the simulation • Winnow is for post-processing

  7. Documentation • Simulation primer • UI Guides for Spider, Kalypso, and Winnow • User Guide • Tutorial

  8. Limitations • Particle energies 0.1 to 100,000 eV • Low energy requires quantum effects • Higher energy requires inelastic reactions

  9. Interactions • SRIM models binary interactions with repulsive potentials • This is most useful for particle energies greater than about 10 eV • Kalypso uses more complete potentials (attractive and repulsive, many-body) • Potentials are cut-off by user (usually 1-2 nearest-neighbors)

  10. Potentials • Use screened coulomb potential splined to attractive portion for short-range interactions • For low energy interactions, use many-body potentials (Sutton-Chen or tight-binding) • Fitting of attractive potential to repulsive portion is not trivial • Many-body potentials improve results near surface and for static properties

  11. Potentials • Many-body potentials are similar to Lennard-Jones potentials • Attractive part of SC is square root of sum of LJ potentials • Attractive part of TB is square root of sum of Morse potentials • Morse potentials:

  12. Choosing Potentials • Choose form of screened coulomb potential (choose screening radius) for both target-target and projectile-target interactions • Choose many-body potential (TB is recommended) • Details (and constants for some materials) are in Simulation Primer

  13. Surface Binding Energy • Many-Body potentials require corrections near surfaces • Pair-potentials alone tend to underestimate surface binding effects • There’s no “best” approach to correcting for surface effects • Current correction in Kalypso reduces perpendicular velocity of emitted particles such that kinetic energy falls by surface binding energy

  14. Thermal Vibrations • Some results will be affected by thermal oscillations of the lattice • Spider calculates mean square thermal vibrations

  15. Electronic Stopping • Several models for electronic stopping are in Kalypso • Described in Simulation Primer • Effects of target temperature are corrected for

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