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Fundamentals of Ion-Solid Interaction - SPIRIT

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<strong>Ion</strong> mixing at precipitates<br />

R<br />

<br />

Atomic relocation<br />

probability per<br />

incident ion<br />

(Assumed to be<br />

isotropic)<br />

w r<br />

<br />

<br />

<br />

exp<br />

<br />

<br />

= (E ion,m ion,m target)<br />

Characteristic Relocation Length<br />

R<br />

Angular and spatial<br />

integration yields radial<br />

relocation field<br />

W r<br />

r<br />

r Atomic relocation is<br />

counteracted by diffusion.<br />

In local equilibrium<br />

K.-H. Heinig et al., Mat.Res.Soc.Proc. vol. 650 (2001)<br />

Institute <strong>of</strong> <strong>Ion</strong> Beam Physics and Materials Research Pr<strong>of</strong>. Wolfhard Möller<br />

r D 2 c<br />

<br />

- r jW<br />

2 r<br />

r r<br />

r<br />

<br />

D Diffusion Coefficient<br />

r j <strong>Ion</strong> Flux<br />

After minor approximations (e.g., r-R > )<br />

<br />

R <br />

<br />

<br />

R <br />

~<br />

c 1 ~<br />

c c R<br />

(Linearized) Gibbs-Thomson<br />

equation holds for ion mixing !<br />

with<br />

c ~<br />

<br />

c<br />

1 <br />

R 5<br />

/<br />

R <br />

1 <br />

~ c<br />

c<br />

<br />

<br />

Dc<br />

q 2<br />

<br />

4<br />

q Nr. <strong>of</strong> displacements per<br />

Atom and Unit <strong>of</strong> Time

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