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Solid state physics
lectures
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fb72477f
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fb72477f
authored
4 years ago
by
Anton Akhmerov
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!104
lecture 10 solutions
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src/10_xray_solutions.md
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fb72477f
...
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@@ -38,11 +38,14 @@ $$
$$
2.
Because the relation between direct and reciprocal lattice is symmetric, so are the expressions for the direct lattice vectors through the reciprocal ones:
$$
\m
athbf{a}_{i}
\e
psilon_{ijk} =
\f
rac{2
\p
i}{V^
*
} (
\m
athbf{b}_{j}
\t
imes
\m
athbf{b}_{k})
$$
where
as
$
\e
psilon_{ijk}$ is the
[
Levi-Civita tensor
](
https://en.wikipedia.org/wiki/Levi-Civita_symbol#Three_dimensions
)
where $
\e
psilon_{ijk}$ is the
[
Levi-Civita tensor
](
https://en.wikipedia.org/wiki/Levi-Civita_symbol#Three_dimensions
)
3.
One set of the BCC primitive lattice vectors is given by:
...
...
@@ -61,7 +64,7 @@ $$
$$
which is forms a reciprocal FCC lattice.
Using the result in Subquestion 2, the vice versa result is trivial
The opposite relation follows directly from our previous result.
4.
Because the 1st Brillouin Zone is the Wigner-Seitz cell of the reciprocal lattice, we need to construct the Wigner-Seitz cell of the FCC lattice.
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