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Analysis of the extended defects in 3C-SiC.pdf - Nelson Mandela ...

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28<br />

The nuclear stopp<strong>in</strong>g power Sn is thus given by <strong>the</strong>se dimensionless parameters as<br />

d<br />

<br />

which is a function <strong>of</strong> ε only. The electronic stopp<strong>in</strong>g power Se is given by,<br />

d<br />

<br />

d<br />

<br />

<br />

d<br />

<br />

n<br />

e<br />

k<br />

1<br />

2<br />

1 2 1 2<br />

3 2<br />

1 0.<br />

0793Z1<br />

Z 2 ( M 1 M 2 )<br />

6<br />

with k Z1<br />

2 3 2 3 3 4 3 2 1 2<br />

( Z1<br />

Z 2 ) M 1 M 2<br />

(3.12)<br />

(3.13)<br />

A universal curve cannot be obta<strong>in</strong>ed for <strong>the</strong> electronic stopp<strong>in</strong>g power s<strong>in</strong>ce k<br />

depends on <strong>the</strong> collid<strong>in</strong>g atoms. Fig. 3.1 shows <strong>the</strong> electronic stopp<strong>in</strong>g power plotted<br />

for two values <strong>of</strong> k be<strong>in</strong>g 1.5 and 0.15. The straight l<strong>in</strong>e <strong>in</strong>dicates <strong>the</strong> dependence on<br />

velocity.<br />

Fig. 3.2. Reduced range-energy plots for various values <strong>of</strong> <strong>the</strong> electronic stopp<strong>in</strong>g<br />

parameter k (from Carter et al. (1976))<br />

The average total path length ρ is <strong>the</strong>n given by,<br />

<br />

<br />

<br />

0<br />

d { S n ( )<br />

S e ( )}<br />

(3.14)

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