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author | Nao Pross <np@0hm.ch> | 2021-05-05 23:07:28 +0200 |
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committer | Nao Pross <np@0hm.ch> | 2021-05-05 23:07:28 +0200 |
commit | 8f862d9be3117979c9694544cca0afa8d2e53cb3 (patch) | |
tree | c432bc839049d35645cb36e3d0596d59154b5da8 | |
parent | Add pauses and minor fixes (diff) | |
download | SeminarMatrizen-8f862d9be3117979c9694544cca0afa8d2e53cb3.tar.gz SeminarMatrizen-8f862d9be3117979c9694544cca0afa8d2e53cb3.zip |
Add (back) slide for algebraic symmetries
Probably won't be used but still.
Diffstat (limited to '')
-rw-r--r-- | vorlesungen/punktgruppen/slides.pdf | bin | 148139 -> 156879 bytes | |||
-rw-r--r-- | vorlesungen/punktgruppen/slides.tex | 51 |
2 files changed, 51 insertions, 0 deletions
diff --git a/vorlesungen/punktgruppen/slides.pdf b/vorlesungen/punktgruppen/slides.pdf Binary files differindex 37ada17..f2af987 100644 --- a/vorlesungen/punktgruppen/slides.pdf +++ b/vorlesungen/punktgruppen/slides.pdf diff --git a/vorlesungen/punktgruppen/slides.tex b/vorlesungen/punktgruppen/slides.tex index cc62969..8edaff6 100644 --- a/vorlesungen/punktgruppen/slides.tex +++ b/vorlesungen/punktgruppen/slides.tex @@ -135,6 +135,57 @@ \section{Algebraische Symmetrien} %% Made in video +\frame{ + \begin{columns}[T] + \begin{column}{.5\textwidth} + Produkt mit \(i\) + \begin{align*} + 1 \cdot i &= i \\ + i \cdot i &= -1 \\ + -1 \cdot i &= -i \\ + -i \cdot i &= 1 + \end{align*} + \pause + % + Gruppe + \begin{align*} + G &= \left\{ + 1, i, -1, -i + \right\} \\ + &= \left\{ + 1, i, i^2, i^3 + \right\} \\ + C_4 &= \left\{ + \mathbb{1}, r, r^2, r^3 + \right\} + \end{align*} + \pause + \end{column} + \begin{column}{.5\textwidth} + Darstellung \(\phi : C_4 \to G\) + \begin{align*} + \phi(\mathbb{1}) &= 1 & \phi(r^2) &= i^2 \\ + \phi(r) &= i & \phi(r^3) &= i^3 + \end{align*} + \pause + % + Homomorphismus + \begin{align*} + \phi(r \circ \mathbb{1}) &= \phi(r) \cdot \phi(\mathbb{1}) \\ + &= i \cdot 1 + \end{align*} + \pause + % + \(\phi\) ist bijektiv \(\implies C_4 \cong G\) + \pause + % + \begin{align*} + \psi : C_4 &\to (\mathbb{Z}/4\mathbb{Z}, +) \\ + \psi(\mathbb{1}\circ r^2) &= 0 + 2 \pmod{4} + \end{align*} + \end{column} + \end{columns} +} \section{3D Symmetrien} %% Made in video |