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Solid state physics
lectures
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66a8e694
Commit
66a8e694
authored
5 years ago
by
Radoica Draškić
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!65
Crystal structure changes
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5 years ago
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66a8e694
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@@ -150,7 +150,7 @@ There is therefore exactly one allowed ${\bf k}$ per volume $\left(\frac{2\pi}{L
When we consider larger and larger box sizes $L→∞$, the volume per allowed mode becomes smaller and smaller, and eventually we obtain an integral:
$$
\s
um_
\m
athbf{k}
\r
ightarrow
\f
rac{L^3}{(2
\p
i)^3}
\i
iint
\l
imits_{-∞}^{∞}dk_x dk_y dk_z
)
\s
um_
\m
athbf{k}
\r
ightarrow
\f
rac{L^3}{(2
\p
i)^3}
\i
iint
\l
imits_{-∞}^{∞}dk_x dk_y dk_z
$$
...
...
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