Stabilizer Code - Mathematical Background

Mathematical Background

The Stabilizer formalism exploits elements of the Pauli group in formulating quantum error-correcting codes. The set consists of the Pauli operators:


I\equiv
\begin{bmatrix}
1 & 0\\
0 & 1
\end{bmatrix}
,\ X\equiv
\begin{bmatrix}
0 & 1\\
1 & 0
\end{bmatrix}
,\ Y\equiv
\begin{bmatrix}
0 & -i\\
i & 0
\end{bmatrix}
,\ Z\equiv
\begin{bmatrix}
1 & 0\\
0 & -1
\end{bmatrix}
.

The above operators act on a single qubit---a state represented by a vector in a two-dimensional Hilbert space. Operators in have eigenvalues and either commute or anti-commute. The set consists of -fold tensor products of Pauli operators:


\Pi^{n}=\left\{
\begin{array}
{c}
e^{i\phi}A_{1}\otimes\cdots\otimes A_{n}:\forall j\in\left\{ 1,\ldots
,n\right\} A_{j}\in\Pi,\ \ \phi\in\left\{ 0,\pi/2,\pi,3\pi/2\right\}
\end{array}
\right\} .

Elements of act on a quantum register of qubits. We occasionally omit tensor product symbols in what follows so that

The -fold Pauli group plays an important role for both the encoding circuit and the error-correction procedure of a quantum stabilizer code over qubits.

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