1 / 16

NEEP 541 – Damage and Displacements

NEEP 541 – Damage and Displacements. Fall 2003 Jake Blanchard. Outline. Damage and Displacements Definitions Models for displacements Damage Efficiency. Definitions. Displacement=lattice atom knocked from its lattice site

elu
Download Presentation

NEEP 541 – Damage and Displacements

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. NEEP 541 – Damage and Displacements Fall 2003 Jake Blanchard

  2. Outline • Damage and Displacements • Definitions • Models for displacements • Damage Efficiency

  3. Definitions • Displacement=lattice atom knocked from its lattice site • Displacement per atom (dpa)=average number of displacements per lattice atom • Primary knock on (pka)=lattice atom displaced by incident particle • Secondary knock on=lattice atom displaced by pka • Displacement rate (Rd)=displacements per unit volume per unit time • Displacement energy (Ed)=energy needed to displace a lattice atom

  4. Formal model • To first order, an incident particle with energy E can displace E/Ed lattice atoms (either itself or through knock-ons) • Details change picture • Let (E)=number of displaced atoms produced by a pka

  5. Formal Model

  6. What is (E) • For T<Ed there are no displacements • For Ed <T<2Ed there is one displacement • Beyond that, assume energy is shared equally in each collision because =1 so average energy transfer is half of the incident energy

  7. Schematic tka ska pka Energy per atom E E/2 E/4 E/2N 2 4 displacements 1 2N

  8. Displacement model • Process stops when energy per atom drops below 2Ed (because no more net displacements can be produced) • So

  9. Kinchin-Pease model  T Ed 2Ed Ec

  10. More Rigorous Approach • Assume binary collisions • No displacements for T>Ec • No electronic stopping for T<Ec • Hard sphere potentials • Amorphous lattice • Isotropic displacement energy • Neglect Ed in collision dynamics

  11. Kinchin-Pease revisited

  12. Kinchin-Pease revisited

  13. Kinchin-Pease revisited • Solution is: • For power law potential, result is:

  14. Electronic Stopping • Repeat with stopping included • Hard sphere potentials Don’t need cutoff energy any more Hard sphere collision cross section (independent of E)

  15. Comprehensive Model • Include all effects (real potential, electronic stopping) • Define damage efficiency:

  16. Damage Efficiency

More Related