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@ -3,9 +3,9 @@
%\usepackage{fullpage}
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@ -17,18 +17,17 @@
\usetikzlibrary{arrows}
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\fancyhead[R]{\footnotesize m-labs.hk}
\fancyhead[L]{
\includegraphics[height=0.16in]{m_labs_logo.pdf}
\includegraphics[height=0.73in]{m_labs_logo_2020.pdf}
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\title{Cheko: high-density electrode driver for scalable ion-trap quantum computing}
\date{November 23, 2020}
\date{December 7, 2020}
\begin{document}
\maketitle
@ -133,7 +132,7 @@ The electrode area of the racetrack ion trap\cite{racetrack} with its 150 region
\end{figure}
\subsection{Temperature range}
Some, but not all, ion trap experiments are done in a cryostat, in particular to reduce ion heating rates and improve vacuum\cite{cryo} (in terms of both pumping speed and ultimate pressure achieved). To address a wider range of ion trap experiments, it is desirable that the device be operable at low temperatures (3 to 10K) as well as room temperature.
Some, but not all, ion trap experiments are done in a cryostat, in particular to reduce ion heating rates and improve vacuum\cite{cryo} (in terms of both pumping speed and ultimate pressure achieved). To address a wider range of ion trap experiments, it is desirable that the device be operable at low temperatures (3 to 15K) as well as room temperature.
\subsection{Vacuum}
The device must be operable in a ultra-high vacuum environment. It must not outgas and must have a sufficient means of dissipating the heat it generates, such as being mounted to the wall of the vacuum chamber acting as heatsink.

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