Add midterm presentation motivation and backup slide

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Andreas Tsouchlos 2026-01-29 00:45:08 +01:00
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[submodule "lib/cel-slides-template-2025"]
path = lib/cel-slides-template-2025
url = git@gitlab.kit.edu:kit/cel/misc/cel-slides-template-2025.git

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\documentclass[overviewatsection, showsubsectionsatfirstoverview]{CELbeamer}
%
%
% CEL Template
%
%
\newcommand{\templates}{preambles}
\input{\templates/packages.tex}
\input{\templates/macros.tex}
\grouplogo{CEL_logo.pdf}
\groupname{Communications Engineering Lab (CEL)}
\fundinglogos{}
%
%
% Document setup
%
%
\usepackage{tikz}
\usepackage{tikz-3dplot}
\usetikzlibrary{spy, external, intersections, positioning}
% \ifdefined\ishandout\else
% \tikzexternalize
% \fi
\usepackage{pgfplots}
\pgfplotsset{compat=newest}
\usepgfplotslibrary{fillbetween}
\usepgfplotslibrary{groupplots}
\usepackage{enumerate}
\usepackage{listings}
\usepackage{subcaption}
\usepackage{bbm}
\usepackage{multirow}
\usepackage{xcolor}
\usepackage{amsmath}
\usepackage{graphicx}
\usepackage{calc}
\usepackage{amssymb}
\usepackage{acro}
\usepackage{braket}
\title{Fault Tolerant Quantum Error Correction}
\subtitle{Master's Thesis Midterm Presentation}
\author[Tsouchlos]{Andreas Tsouchlos}
\date[]{February 5th, 2026}
\DeclareFieldFormat{note}{}
\DeclareFieldFormat{issn}{}
\DeclareFieldFormat{url}{}
\DeclareFieldFormat{doi}{}
\DeclareFieldFormat[article,book,inproceedings]{urldate}{}
\addbibresource{MA.bib}
%
%
% Custom commands
%
%
\newcommand{\res}{src/midterm_presentation/res}
%
%
% Acronyms
%
%
\DeclareAcronym{qec}{
short=QEC,
long=quantum error correction
}
%
%
% Document body
%
%
\begin{document}
\begin{frame}[title white vertical, picture=images/IMG_7801-cut]
\titlepage
\end{frame}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\section{Introduction to Quantum Error Correction}
\label{sec:Introduction to Quantum Error Correction}
%%%%%%%%%%%%%%%%
\subsection{Motivation}
\label{subsec:Motivation}
\begin{frame}
\frametitle{Quantum Computing}
% Related interesting stuff
% - Gidney estimates we need 1399 (?) logical qubits to factor a 2048
% bit RSA integer
% - He goes on to estimate that to factor such an integer in less
% than a week would require around a million physical qubits
% [How to factor 2048 bit RSA integers with less than a million
% noisy qubits]
\vspace*{-19mm}
\begin{itemize}
\item Simulating quantum systems on classical hardware
is exponentially complex \\
$\rightarrow$ Can't we use quantum hardware to simulate
quantum systems? \citereference{feynman_simulating_1982}
\item Some problems that are ``hard'' to solve on classical
computers we can ``easily'' solve on quantum computers
\citereference{preskill_quantum_2018}
\item We are still in the early days of quantum computing
\end{itemize}
\vspace*{-5mm}
\begin{figure}[H]
\centering
\includegraphics[scale=0.43]{res/google_roadmap.png}
\vspace*{-3mm}
\caption{
Google Quantum AI's quantum computing roadmap
\citereference{google_quantum_ai_quantum_nodate}.
}
\end{figure}
\addreferences
{feynman_simulating_1982}
{preskill_quantum_2018}
{google_quantum_ai_quantum_nodate}
\stopreferences
\end{frame}
% TODO: Where should I quote Preskill? There are multiple bullet
% points with info taken from his work
\begin{frame}
\frametitle{The Need for Quantum Error Correction}
\vspace*{-10mm}
% Related interesting stuff
% - Qubits differ from bits in that they can be in superpositions
% and be entangled with one another
% - Quantum computers derive their strenght from the exponential
% scaling of the state-space because of the way the information is
% encoded
% - Note that while a physical error rate of 10^{-3} may seem ok,
% we need a couple trillion operations (~ 10^{13}) to factor a
% 2048 bit RSA integer
% [How to factor 2048 bit RSA integers with less than a million
% noisy qubits]
% - The backlog problem is the fact that an increasing backlog of
% syndrome data will lead to an exponential slowdown during the
% computation
\begin{itemize}
\item Quantum computers represent information through
correlations of qubits, not their values \\
directly \citereference{preskill_quantum_2018}
\item We want to not disturb the quantum state but need to
interact with the system \\
$\rightarrow$ Protect the state with \ac{qec}
\item We employ more physical qubits to introduce
redundancy and use the resulting \emph{physical} state to
represent the \emph{logical} state
\citereference{roffe_quantum_2019}
\item IBM recently introduced a scheme encoding 12 logical
qubits in 288 physical ones
\citereference{bravyi_high-threshold_2024}
\item The physical error rate is typically assumed to be $10^{-3}$ for
simulations (e.g., \citereference{bravyi_high-threshold_2024})
\item Decoding has to happen with ultra-low latency to avoid
the backlog problem (about $\SI{1}{us}$ per data
extraction round) \citereference{caune_demonstrating_2024}
% \citereference{terhal_quantum_2015}
\end{itemize}
\vspace*{12mm}
\addreferences
% {terhal_quantum_2015}
{caune_demonstrating_2024}
{preskill_quantum_2018}
{roffe_quantum_2019}
{bravyi_high-threshold_2024}
\stopreferences
\end{frame}
%%%%%%%%%%%%%%%%
\subsection{Fundamentals of Quantum Error Correction}
\label{subsec:Fundamentals of Quantum Error Correction}
% TODO: Is this all of this really necessary?
\begin{frame}
\frametitle{Peculiarities of the Quantum Setting}
% Related interesting stuff
% - No cloning theorem -> Not replication of state, protection
% through further entanglement
% - States are superpositions -> We theoretically need to be able
% to correct infinitely many different types of errors. Luckily,
% it turns out that in actual fact we only really need to correct
% two [Gottesman's Thesis]
\begin{itemize}
\item Measuring the system collapses the quantum state
$\rightarrow$ Loss of benefit of quantum system \\
$\rightarrow$ For BP, we work with the syndrome and not
the variable nodes \textcolor{red}{This can't be here,
it's before introducing how QEC works}
\item X and Z errors
\item With QEC we are able to restore the quantum state, not
"just the bits"
\item We don't care about the specific error, only the coset
its in $\rightarrow$ We only really care about the syndrome
\end{itemize}
\end{frame}
\begin{frame}
\frametitle{Fundamentals of Quantum Error Correction}
\begin{itemize}
\item Stabilizer codes: the quantum equivalent of binary linear codes
\item CSS codes: separate corection of X and Z errors
$\rightarrow$ simpler circuitry
\item Construction of CSS codes from binary linear codes
\textcolor{red}{Is this really necessary?}
\end{itemize}
\end{frame}
% TODO: Is this really necessary?
\begin{frame}
\frametitle{The Quantum Error Correction Landscape}
\begin{itemize}
\item Give basic overview of most promising avenues of
research (as in ECCentric paper)
\end{itemize}
\end{frame}
\begin{frame}
\frametitle{An Example: The Steane Code}
\begin{itemize}
\item \textcolor{red}{Give example slides grey background or something?}
\item The Steane code is the quantum equivalent of the
[7,4]-Hamming code
\item Construction from Hamming code
\item Syndrome Extraction Circuitry
\end{itemize}
\end{frame}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\section{Fault Tolerance and Detector Error Models}
\label{sec:Fault Tolerance and Detector Error Models}
%%%%%%%%%%%%%%%%
\subsection{Fault Tolerance}
\label{subsec:Fault Tolerance}
\begin{frame}
\frametitle{Fault Tolerance}
\begin{itemize}
\item Quantum gates are faulty $\rightarrow$ we need QEC \\
But we do QEC with faulty gates $\rightarrow$ we need
fault tolerant QEC %
\footnote{
Designing fault-tolerant circuits using detector
error models - Gong et al, Section 4.1
}
\item We generally do multiple rounds of syndrome extraction
\item The Threshold theorem
\setcounter{footnote}{0}
\item Definition of fault tolerance \footnotemark
\item \textcolor{red}{Different approaches to fault tolerance?}
\end{itemize}
\end{frame}
%%%%%%%%%%%%%%%%
\subsection{Detector Error Models}
\label{subsec:Detector Error Models}
\begin{frame}
\frametitle{Detector Error Models}
\begin{itemize}
\item Idea: Go "one layer of abstraction higher" \\
$\rightarrow$ Redefine syndrome and create new PC matrix from that
\end{itemize}
\end{frame}
\begin{frame}
\frametitle{An Example: Steane Code Detector Error Model}
\begin{itemize}
\item New Syndrome Extraction Circuitry \textcolor{red}{Is a
repetition of the old circuitry needed?}
\item New parity check matrix
\item Highlighting of the SC-LDPC-code-like structure
\end{itemize}
\end{frame}
\begin{frame}
\frametitle{Challenges}
\begin{itemize}
\item Multiple different errors are summarized $\rightarrow$
short cycles \& degeneracy
\footnote{
\texttt{
https://www.math.cit.tum.de/fileadmin/w00ccg/math/\_my\_direct\_uploads/Dan\_Browne.pdf
}
}
\\
$\rightarrow$ We generally don't use "normal BP" (BP +
OSD, BPGD, etc.)
\end{itemize}
\end{frame}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\section{State of the Art and Research Gap}
\label{sec:State of the Art and Research Gap}
%%%%%%%%%%%%%%%%
\subsection{State of the Art}
\label{subsec:State of the Art}
\begin{frame}
\frametitle{Sliding Window Decoding}
\begin{itemize}
\item Give overview of existing research
\item Explain exactly what they do in the main paper I am
basing my work on
\end{itemize}
\end{frame}
\begin{frame}
\frametitle{Guided Decimation Guessing Decoding}
\begin{itemize}
\item Update equations
\item Key ideas
\item Syndrome Based BP
\end{itemize}
\end{frame}
\begin{frame}
\frametitle{Memory experiments}
\begin{itemize}
\item What is a memory experiment?
\item Communications Engineering view (what are my inputs and
outpus? What do I expect?)
\end{itemize}
\end{frame}
\begin{frame}
\frametitle{Systemic overview}
\begin{itemize}
\item Top level overview of entire system: X and Z syndrome
extraction, logical operator measurement, where decoding
takes place, etc.
\end{itemize}
\end{frame}
\begin{frame}
\frametitle{Research Gap}
\begin{itemize}
\item Use soft information for sliding window decoding
$\rightarrow$ Treat as spacially coupled LDPC code
\item Current work considers X and Z errors separately
(probably for latency reasons) $\rightarrow$ See how
decoding the jointly works out
\end{itemize}
\end{frame}
%%%%%%%%%%%%%%%%
\subsection{What we simulate}
\label{subsec:What we simulate}
\begin{frame}
\frametitle{The lack of a Standard Evaluation System}
\begin{itemize}
\item \textcolor{red}{Look into ECCentric}
\item There is not even a standard figure of merit (e.g.,
FER/BER over SNR in classical case) $\rightarrow$
Multiple different kinds of plots (e.g., footprint)
\item Overview of variables
\end{itemize}
\end{frame}
\begin{frame}
\frametitle{Proposed Evaluation Pipeline}
\begin{itemize}
\item To what values I will fix the parameters and why
\item What figure of merit I will use and why
\end{itemize}
\end{frame}
\appendix
\beginbackup
\begin{frame}
\frametitle{System Level Overview}
\vspace*{-15mm}
\begin{figure}[H]
\centering
\begin{subfigure}[t]{0.5\textwidth}
\centering
\includegraphics[scale=1.1]{res/architecture}
\vspace*{5mm}
\caption{Schematic workflow of surface code quantum
computation \citereference{zhang_classical_2023}.}
\end{subfigure}%
\begin{subfigure}[t]{0.5\textwidth}
\centering
\tikzset{
block/.style={
draw, rectangle,
fill = kit-blue!25,
minimum width=75mm, minimum height=15mm,
}
}
\scalebox{0.7}{
\begin{tikzpicture}[node distance=15mm and 20mm]
\node[block] (encoding) {Encoding};
\node[block, below=of encoding] (channel) {Quantum Channel};
\node[block, below=of channel] (reverse-op)
{Reverse Operation};
\node[block, right=of channel] (syn-extr)
{Syndrome Extraction};
\node[block, below=of syn-extr] (syn-dec)
{Syndrome Decoder};
\node[above=of encoding] (input) {$\ket{\phi}$};
\node[below=of reverse-op] (output)
{$\hat{\mathcal{E}}\mathcal{E}\ket{\psi}$};
\draw [-{Latex}] (encoding) -- (channel) node[midway,
right] {$\ket{\psi}$};
\draw [-{Latex}] (channel) -- (reverse-op)
node[midway, right] {$\mathcal{E}\ket{\psi}$};
\draw [-{Latex}] (channel) -- (syn-extr)
node[midway, above] {$\mathcal{E}\ket{\psi}$};
\draw [-{Latex}] (syn-extr) -- (syn-dec)
node[midway, right] {$z$};
\draw [-{Latex}] (syn-dec) -- (reverse-op)
node[midway, above] {$\hat{\mathcal{E}}$};
\draw [-{Latex}] (input) -- (encoding);
\draw [-{Latex}] (reverse-op) -- (output);
\end{tikzpicture}
}
\vspace*{5mm}
\caption{Block diagram of QEC using stabilizer codes
\citereference{miao_quaternary_2025}.}
\end{subfigure}
\end{figure}
% \vspace*{-2mm}
\addreferences
{zhang_classical_2023}
{miao_quaternary_2025}
\stopreferences
\end{frame}
\backupend
\end{document}

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