fixed some stuff as suggested by Simon

thesis/chapters/quantum_computing.tex

@@ -96,7 +96,7 @@ integer states
 
 \begin{equation}
     \label{eq:ci}
-    \ket{\psi} = \sum\limits_{i = 0}^{2^n - 1} c_i \ket{i} .
+    \ket{\psi} = \sum\limits_{i = 0}^{2^n - 1} c_i \ket{i}
 \end{equation}
 
 with the normation condition
@@ -176,13 +176,13 @@ The matrix representation of $CX$ and $CZ$ for two qbits is given by
 
 \begin{postulate}
     Let 
-    $$\ket{\psi} = \alpha\ket{\phi_1} \otimes \ket{1}_j + \beta\ket{\phi_0} \otimes \ket{0}_j$$ 
+    \begin{equation}\ket{\psi} = \alpha\ket{\phi_1} \otimes \ket{1}_j + \beta\ket{\phi_0} \otimes \ket{0}_j\end{equation} 
     be a  $n$-qbit state
     where $\ket{1}_j, \ket{0}_j$ denote the $j$-th qbit state and $|\alpha|^2 + |\beta|^2 = 1$. 
     Then the measurement of the $j$-th qbit will yield 
-    $$\ket{\phi_1} \otimes \ket{1}_j$$ 
+    \begin{equation}\ket{\phi_1} \otimes \ket{1}_j\end{equation} 
     with probability $|\alpha|^2$ and 
-    $$\ket{\phi_0} \otimes \ket{0}_j$$
+    \begin{equation}\ket{\phi_0} \otimes \ket{0}_j\end{equation}
     with probability $|\beta|^2$ \cite{nielsen_chuang_2010}.  This is called collapse of the wave function.
 \end{postulate}
 

thesis/main.tex

@@ -39,7 +39,8 @@
 \title{An Efficient Quantum Computing Simulator using a Graphical Description for Many-Qbit Systems \\
 \large Bachelor Thesis}
 \author[1]{Daniel Knüttel}
-\affil[1]{Institute I - Theoretical Physics, University of Regensburg}
+\affil[1]{Institute I - Theoretical Physics, University of Regensburg\\
+Supervised by Prof. Dr. Christoph Lehner}
 \date{10.04.2020} 
 \begin{document} 
 \maketitle