Final readthrough corrections for fault tolerance chapter
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@@ -16,19 +16,19 @@ using qubits.
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While the use of error correcting codes may facilitate this, it also
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While the use of error correcting codes may facilitate this, it also
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introduces two new challenges \cite[Sec.~4]{gottesman_introduction_2009}:
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introduces two new challenges \cite[Sec.~4]{gottesman_introduction_2009}:
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\begin{itemize}
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\begin{itemize}
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\item For realizing a quantum algorithm, we must be able to
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\item To realize a quantum algorithm, we must be able to
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perform operations on the encoded state in such a way that we
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perform operations on the encoded state in such a way that we
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do not lose the protection against errors.
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do not lose the protection against errors.
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\item \ac{qec} systems, in particular the syndrome extraction
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\item \ac{qec} systems, in particular the syndrome extraction
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circuit, are themselves partially implemented in
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circuit, are themselves partially implemented in
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quantum hardware.
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quantum hardware.
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In addition to the errors we have originally introduced them
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In addition to the errors we have originally introduced them
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for, these systems must be able to account for the fact they
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for, these systems must therefore be able to account for the
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are implemented on noisy hardware themselves.
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fact they are implemented on noisy hardware themselves.
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\end{itemize}
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\end{itemize}
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In the literature, both of these points are viewed under the umbrella
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In the literature, both of these points are viewed under the umbrella
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of \emph{fault-tolerant} quantum computing.
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of \emph{fault-tolerant} quantum computing.
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In this thesis, we focus only on the second aspect.
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In this thesis, we focus on the second aspect.
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It was recognized early on as a challenge of \ac{qec} that the correction
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It was recognized early on as a challenge of \ac{qec} that the correction
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machinery itself may introduce new faults \cite[Sec.~III]{shor_scheme_1995}.
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machinery itself may introduce new faults \cite[Sec.~III]{shor_scheme_1995}.
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@@ -938,10 +938,10 @@ triggered the measurements in the syndrome extraction round immediately
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afterwards, but all subsequent ones as well.
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afterwards, but all subsequent ones as well.
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To only see the effect of errors in the syndrome measurement round
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To only see the effect of errors in the syndrome measurement round
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immediately following them, we consider our newly defined detectors
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immediately following them, we consider our newly defined detectors
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instead of the measurements, that effectively compute the difference
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instead of the measurements.
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between the measurements.
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These effectively compute the difference between the measurements.
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Hereby, each error can only trigger syndrome bits that follow it.
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Each error can only trigger syndrome bits that follow it.
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This is reflected in the triangular structure of $\bm{\Omega}$ in
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This is reflected in the triangular structure of $\bm{\Omega}$ in
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\Cref{eq:syndrome_matrix_ex}.
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\Cref{eq:syndrome_matrix_ex}.
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Combining the measurements into detectors according to
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Combining the measurements into detectors according to
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@@ -1121,7 +1121,7 @@ In fact, it was in this tool that the concept of the \ac{dem} was
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first introduced.
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first introduced.
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One capability of stim, and \acp{dem} in general, that we did not
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One capability of stim, and \acp{dem} in general, that we did not
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explain in detail about in this chapter, is the merging of error mechanisms.
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explain in detail in this chapter, is the merging of error mechanisms.
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Since \acp{dem} differentiate errors based on their effect on the
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Since \acp{dem} differentiate errors based on their effect on the
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measurements and not on their Pauli type and location
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measurements and not on their Pauli type and location
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\cite[Sec.~1.4.3]{higgott_practical_2024}, it is natural to group
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\cite[Sec.~1.4.3]{higgott_practical_2024}, it is natural to group
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