Adds figures wrt T

paper.tex

@@ -260,6 +260,93 @@ In this regime, Johnson noise no longer becomes an issue for these qubits.
 \end{itemize}
 \section{Conclusions \label{sec:conclusions}}
 
+\section{Additional Figures}
+
+Slices of \cref{fig:Cliff} are plotted for different frequencies in \crefrange{fig:omega:5}{fig:omega:85}, to better show the behaviour of the cliff-edge.
+Additionally, we have plotted different values of the impurity collision frequency $\tau$, to show how dirtier superconductors, with smaller $\tau$, have much higher values for the noise.
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constOmega/5.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $\omega$.} \label{fig:omega:5}
+\end{figure}
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constOmega/15.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $\omega$.} \label{fig:omega:15}
+\end{figure}
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constOmega/25.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $\omega$.} \label{fig:omega:25}
+\end{figure}
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constOmega/35.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $\omega$.} \label{fig:omega:35}
+\end{figure}
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constOmega/45.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $\omega$.} \label{fig:omega:45}
+\end{figure}
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constOmega/55.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $\omega$.} \label{fig:omega:55}
+\end{figure}
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constOmega/65.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $\omega$.} \label{fig:omega:65}
+\end{figure}
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constOmega/75.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $\omega$.} \label{fig:omega:75}
+\end{figure}
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constOmega/85.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $\omega$.} \label{fig:omega:85}
+\end{figure}
+
+Similarly, we can make slices of \cref{fig:Cliff} for constant temperature, and show how the noise drops off for a different frequency.
+These slices are plotted in \crefrange{fig:T:10}{fig:T:40}.
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constT/10.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $T$.} \label{fig:T:10}
+\end{figure}
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constT/20.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $T$.} \label{fig:T:20}
+\end{figure}
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constT/30.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $T$.} \label{fig:T:30}
+\end{figure}
+
+\begin{figure}[htp]
+	\centering
+	\includegraphics[width=12cm]{constT/40.jpg}
+	\caption{A slice of \cref{fig:Cliff} for constant $T$.} \label{fig:T:40}
+\end{figure}
+
+
 \printbibliography
 
 \end{document}