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authorAndreas Müller <andreas.mueller@ost.ch>2021-02-22 11:05:22 +0100
committerAndreas Müller <andreas.mueller@ost.ch>2021-02-22 11:05:22 +0100
commit57839140bd44eba59e578e055f8a7720ea1a0865 (patch)
tree4d9947e3e0c99e3b31e38d83f3c0f873ae51b8fc /vorlesungen/slides/1
parentstream stuff (diff)
downloadSeminarMatrizen-57839140bd44eba59e578e055f8a7720ea1a0865.tar.gz
SeminarMatrizen-57839140bd44eba59e578e055f8a7720ea1a0865.zip
slides
Diffstat (limited to 'vorlesungen/slides/1')
-rw-r--r--vorlesungen/slides/1/dreieck.tex14
-rw-r--r--vorlesungen/slides/1/speziell.tex1
2 files changed, 11 insertions, 4 deletions
diff --git a/vorlesungen/slides/1/dreieck.tex b/vorlesungen/slides/1/dreieck.tex
index f4909e2..f38f78d 100644
--- a/vorlesungen/slides/1/dreieck.tex
+++ b/vorlesungen/slides/1/dreieck.tex
@@ -30,21 +30,25 @@ U&=
\end{block}
\end{column}
\begin{column}{0.31\textwidth}
+\uncover<2->{%
\begin{block}{Nilpotente Matrix}
\[
N=
\begin{pmatrix}
-*&*&*&\dots&*\\
0&*&*&\dots&*\\
0&0&*&\dots&*\\
+0&0&0&\dots&*\\
\vdots&\vdots&\vdots&\ddots&\vdots\\
-0&0&0&\dots&*
+0&0&0&\dots&0
\end{pmatrix}
\]
+\uncover<3->{%
$\Rightarrow N^n=0$
-\end{block}
+}
+\end{block}}
\end{column}
\begin{column}{0.31\textwidth}
+\uncover<4->{%
\begin{block}{Jordan-Matrix}
\[
J_\lambda=\begin{pmatrix}
@@ -55,8 +59,10 @@ J_\lambda=\begin{pmatrix}
0&0&0&\dots&\lambda
\end{pmatrix}
\]
+\uncover<5->{%
$\Rightarrow J_\lambda -\lambda I$ ist nilpotent
-\end{block}
+}
+\end{block}}
\end{column}
\end{columns}
\end{frame}
diff --git a/vorlesungen/slides/1/speziell.tex b/vorlesungen/slides/1/speziell.tex
index 87b767a..83b3735 100644
--- a/vorlesungen/slides/1/speziell.tex
+++ b/vorlesungen/slides/1/speziell.tex
@@ -37,6 +37,7 @@ AI=IA=A
\end{block}
\begin{block}{Hadamard-Algebra}
Die Algebra der Diagonalmatrizen ist die Hadamard-Algebra
+(siehe später)
\end{block}
\end{column}
\end{columns}