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