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Stabilizer code : ウィキペディア英語版
Stabilizer code

The theory of quantum error correction plays a prominent role in the practical realization and engineering of
quantum computing and quantum communication devices. The first quantum
error-correcting codes are strikingly similar to classical block codes in their
operation and performance. Quantum error-correcting codes restore a noisy,
decohered quantum state to a pure quantum state. A
stabilizer quantum error-correcting code appends ancilla qubits
to qubits that we want to protect. A unitary encoding circuit rotates the
global state into a subspace of a larger Hilbert space. This highly entangled,
encoded state corrects for local noisy errors. A quantum error-correcting code makes quantum computation
and quantum communication practical by providing a way for a sender and
receiver to simulate a noiseless qubit channel given a noisy qubit channel
that has a particular error model.
The stabilizer theory of quantum error correction allows one to import some
classical binary or quaternary codes for use as a quantum code. The only
"catch" when importing is that the
classical code must satisfy the dual-containing or self-orthogonality
constraint. Researchers have found many examples of classical codes satisfying
this constraint, but most classical codes do not. Nevertheless, it is still useful to import classical codes in this way (though, see how the entanglement-assisted stabilizer formalism overcomes this difficulty).
== Mathematical background ==

The Stabilizer formalism exploits elements of
the Pauli group \Pi in formulating quantum error-correcting codes. The set
\Pi=\left\ consists of the Pauli operators:
:
I\equiv
\begin
1 & 0\\
0 & 1
\end
,\ X\equiv
\begin
0 & 1\\
1 & 0
\end
,\ Y\equiv
\begin
0 & -i\\
i & 0
\end
,\ Z\equiv
\begin
1 & 0\\
0 & -1
\end
.

The above operators act on a single qubit---a state represented by a vector in a two-dimensional
Hilbert space. Operators in \Pi have eigenvalues \pm1 and either commute
or anti-commute. The set \Pi^ consists of n-fold tensor products of
Pauli operators:
:
\Pi^=\left\
e^A_\otimes\cdots\otimes A_:\forall j\in\left\ A_\in\Pi,\ \ \phi\in\left\
\end
\right\} .

Elements of \Pi^ act on a quantum register of n qubits. We
occasionally omit tensor product symbols in what follows so that
:A_\cdots A_\equiv A_\otimes\cdots\otimes A_.
The n-fold Pauli group
\Pi^ plays an important role for both the encoding circuit and the
error-correction procedure of a quantum stabilizer code over n qubits.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「Stabilizer code」の詳細全文を読む



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