From 8b12452157b8ee82d1d9d72c16aa868880746e36 Mon Sep 17 00:00:00 2001
From: =?UTF-8?q?Daniel=20Kn=C3=BCttel?= <daniel.knuettel@daknuett.eu>
Date: Mon, 9 Mar 2020 16:41:26 +0100
Subject: [PATCH] added some more stuff

---
 presentation/main.tex | 15 ++++++++++++++-
 1 file changed, 14 insertions(+), 1 deletion(-)

diff --git a/presentation/main.tex b/presentation/main.tex
index b4be715..f462672 100644
--- a/presentation/main.tex
+++ b/presentation/main.tex
@@ -844,7 +844,18 @@
 \end{frame}
 }
 
-\section{Limitations and Future Work}
+\section{Conclusion and Outlook}
+
+{
+\begin{frame}{Properties of Stabilizer States}
+    \begin{itemize}
+        \item{Stabilizer states support entanglement; One example is the Bell state $\frac{\ket{\mbox{0b}00} + \ket{\mbox{0b}11}}{\sqrt{2}}$.}
+        \item{Some forms of superposition exist in the stabilizer formalism.}
+        \item{Stabilizer states and their dynamics (including measurement) can be simulated exponentiallly faster than dense state vectors.}
+    \end{itemize}
+
+\end{frame}
+}
 
 {
 \begin{frame}{Non-Universality}
@@ -907,6 +918,8 @@
             holds. The Pauli matrices are one group that fulfills this property.
             }
 
+        \item{It is not immideately clear how measurement would work.}
+
     \end{itemize}
 \end{frame}
 }