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The geometry factor (always for a
single vacancy) was defined as |
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With Δxi = component of the jump in
x-direction. |
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Looking at the fcc lattice we realize that there
are 12 possibilities for a jump because there are 12 next
neighbors. |
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8 of the possible jumps have
a component in x (or x ) -direction, and
Δxi = a/2 |
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We thus have |
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g fcc |
= ½ · |
8 · |
( |
1
2 |
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2 |
= 1 |
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Looking at the bcc lattice we realize that there
are 8 possibilities for a jump because there are 8 next
neighbors. |
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All 8 possible jumps have the component
Δxi = a/2 in
x-direction, again we have |
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g bcc |
= ½ · |
8 · |
( |
1
2 |
) |
2 |
= 1 |
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Looking at the
diamond
lattice we realize, after a bit more thinking (or drawing, or looking at a
ball and stick model), that there are 4 possible jumps. |
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All 4 jumps have the component Δxi = a/4 in
x-direction, and we obtain |
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g diamond |
= ½ · |
4 · |
( |
1
4 |
) |
2 |
= 1/8 |
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© H. Föll