 |
Essentially we have two rather direct
methods |
|
| 3 |
æ
ç
è |
Dl
l |
|
Da
a |
ö
÷
ø |
= |
cV
ci |
|
 |
|
|
 |
Differential Thermal Expansion (or Dl/ l- Da/a -method). |
|
|
 |
.Positron annihilation |
|
 |
Both methods will not give results if
the vacancy concentration at the melting point is below, roughly,
107. |
|
|
|
|
|
|
|
| <t> |
= |
t2 · |
1 + t2n · cV
1 + t1n ·
cV |
|
|
|
|
|
|
|
 |
Most numbers for point defects in
metals and some other crystals were obtained by these two methods. |
|
| |
|
|
|
 |
There are many other methods, but
always either limited to certain crystals, expensive, hard to evaluate, and so
on. |
|
|
 |
In essence, there are still no
reliable and undisputed numbers for, e.g., the formation and migration
enthalpies for vacancies (and interstitials) in Si or other
semiconductors like GaAs. |
|
|
|
|
|
|
|
© H. Föll (Defects - Script)