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Copy file name to clipboardExpand all lines: codes/quantum/properties/hamiltonian/constant_excitation.yml
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features:
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rate: 'Fock-state CE codes can be used in a protocol that achieves the two-way quantum capacity of the \hyperref[topic:ad]{AD} Gaussian channel \cite{arxiv:2203.13924}. For every \(K,t \geq 2\), there are explicitly constructible \(K\)-dimensional Fock-state CE codes with \(q=N=(K-1)t(t+1)\) modes, total excitation \(N\), and distance \(t+1\); there also exist families with logical dimension \(K = o(2^N)\) and distance of \hyperref[topic:asymptotics]{order} \(o(N/\log N)\) \cite{arxiv:2509.20545}.'
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fault_tolerance:
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- 'Fault-tolerant QEC framework for CE CSS codes using modified Shor and Steane syndrome extraction, where weight-\(2w\) stabilizers are measured using \(w\)-CE cat states and zero-controlled NOT (\(\mathrm{C}_0 X\)) gates replace standard CNOT gates to preserve the constant-excitation structure \cite{arxiv:2507.10395}.'
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parents:
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Qubit CE codes are protected from coherent noise in the form of transversal \(Z\)-rotations because such rotations act identically on all codewords \cite{doi:10.1109/ISIT45174.2021.9518206,arxiv:2011.00197}.
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In the case of qubit CSS codes, all codes oblivious to such rotations are CE codes \cite{doi:10.1109/ISIT45174.2021.9518206,arxiv:2011.00197}.
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Any \([[n,k,d]]\) CSS code can be made into an \([[mn,k,>d]]\) CE code \cite{doi:10.1109/ISIT45174.2021.9518206}.
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Concatenating the dual-rail code with an inner \([[n,k,d]]\) qubit stabilizer code yields a degenerate \([[2n,k,d]]\) constant-excitation stabilizer code that avoids coherent phase errors and is equivalent to a Pauli-rotated repetition-concatenated stabilizer code \cite{arxiv:2010.00538}. CSS structure is preserved when the original code is CSS \cite{arxiv:2507.10395}.
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- code_id: stab_5_1_3
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detail: 'The five-qubit code can be concatenated with a particular decoherence-free subspace (DFS) \cite{arxiv:quant-ph/9807004,arxiv:quant-ph/9902041,arxiv:quant-ph/9908064,arxiv:quant-ph/0007013} to yield a 20-qubit CE code \cite{arxiv:quant-ph/9809081,arxiv:quant-ph/9907096}.'
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detail: 'The five-qubit code can be concatenated with a particular decoherence-free subspace (DFS) \cite{arxiv:quant-ph/9807004,arxiv:quant-ph/9902041,arxiv:quant-ph/9908064,arxiv:quant-ph/0007013} to yield a 20-qubit CE code \cite{arxiv:quant-ph/9809081,arxiv:quant-ph/9907096}. Dual-rail concatenation of the five-qubit code yields a \([[10,1,3]]\) CE stabilizer code \cite{arxiv:2507.10395}.'
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- code_id: qubit_stabilizer
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detail: 'Concatenating the dual-rail code with an inner \([[n,k,d]]\) qubit stabilizer code yields a degenerate \([[2n,k,d]]\) constant-excitation stabilizer code that avoids coherent phase errors and is equivalent to a Pauli-rotated repetition-concatenated stabilizer code \cite{arxiv:2010.00538}. CSS structure is preserved when the original code is CSS \cite{arxiv:2507.10395}.'
Twelve-qubit constant-excitation (CE) CSS code that encodes one logical qubit with distance three.
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It is the smallest CE CSS code that corrects a single-qubit error \cite{arxiv:2507.10395}.
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Codewords lie in a fixed Hamming-weight subspace, making the code immune to coherent noise in the form of transversal \(Z\)-rotations.
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One stabilizer tableau for the code is, up to Pauli frame \cite{arxiv:2507.10395},
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\begin{align}
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\begin{smallmatrix}
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X & X & X & X & I & I & I & I & I & I & I & I \\
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I & I & X & X & X & X & I & I & I & I & I & I \\
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I & I & I & I & I & I & X & X & X & X & I & I \\
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I & I & I & I & I & I & I & I & X & X & X & X \\
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Z & I & Z & I & Z & I & Z & I & Z & I & Z & I \\
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Z & Z & I & I & I & I & I & I & I & I & I & I \\
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I & I & Z & Z & I & I & I & I & I & I & I & I \\
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I & I & I & I & Z & Z & I & I & I & I & I & I \\
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I & I & I & I & I & I & Z & Z & I & I & I & I \\
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I & I & I & I & I & I & I & I & Z & Z & I & I \\
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I & I & I & I & I & I & I & I & I & I & Z & Z
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\end{smallmatrix}~.
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\end{align}
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protection: |
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Corrects any single-qubit error (distance \(d=3\)).
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Protects from collective coherent noise in the form of transversal \(Z\)-rotations, since all codewords lie in the same Hamming-weight subspace \cite{doi:10.1109/ISIT45174.2021.9518206,arxiv:2011.00197}.
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features:
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fault_tolerance:
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- 'Fault-tolerant syndrome extraction using modified Shor and Steane methods adapted for CE codes: weight-\(2w\) stabilizers are measured using \(w\)-CE cat states, and zero-controlled NOT (\(\mathrm{C}_0 X\)) gates replace standard CNOT gates to preserve the constant-excitation structure \cite{arxiv:2507.10395}.'
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threshold:
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- 'Pseudo-threshold of \(\sim 9.28 \times 10^{-4}\) (circuit-level stochastic noise) and \(\sim 5.98 \times 10^{-4}\) (with coherent corrections, \(\gamma = 0.01\)) under collective coherent noise \cite{arxiv:2507.10395}.'
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relations:
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parents:
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- code_id: qubit_css
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- code_id: constant_excitation
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- code_id: qubit_concatenated
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detail: 'This code is obtained by dual-rail concatenation of the \([[6,1,2]]\) CSS code \cite[ID 50]{preset:qiskit}.'
CSS phantom code obtained by concatenating the \([[7,3,(d_X=3,d_Z=2)]]\) punctured hypercube code with the two-qubit phase-flip repetition code.
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The code is equivalent to the \([[14,3,3]]\) constant-excitation (CE) CSS code obtained by applying dual-rail concatenation to the \([[7,3,2]]\) punctured hypercube code, up to single-qubit Clifford gates, a physical-qubit permutation, and a Pauli frame \cite{arxiv:2507.10395}.
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One stabilizer tableau for the code is
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\begin{align}
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- 'The code is phantom, so every ordered-pair in-block logical CNOT gate between its three logical qubits can be implemented by a physical-qubit permutation \cite{arxiv:2601.20927}.'
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- 'The Hadamard-dual code admits fold-diagonal logical \(S_iS_j\) and \(CZ_{ij}\) gates \cite{arxiv:2601.20927}.'
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fault_tolerance:
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- 'In the locally Clifford-equivalent CE CSS frame, fault-tolerant syndrome extraction can use modified Shor and Steane methods adapted for CE codes: weight-\(2w\) stabilizers are measured using \(w\)-CE cat states, and zero-controlled NOT (\(\mathrm{C}_0 X\)) gates replace standard CNOT gates to preserve the constant-excitation structure \cite{arxiv:2507.10395}.'
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- code_id: phantom
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detail: 'This \([[14,3,3]]\) code is a CSS phantom code obtained from the punctured hypercube code and the two-qubit phase-flip repetition code \cite{arxiv:2601.20927}.'
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- code_id: constant_excitation
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detail: 'This code is single-qubit Clifford equivalent to the \([[14,3,3]]\) CE CSS code obtained by dual-rail concatenation of the \([[7,3,2]]\) punctured hypercube code \cite{arxiv:2507.10395}.'
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- code_id: qubit_concatenated
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detail: 'This code is a concatenation of the \([[7,3,2]]\) punctured hypercube code with the two-qubit phase-flip repetition code \cite{arxiv:2601.20927}.'
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- code_id: small_distance_qubit_stabilizer
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cousins:
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- code_id: xz_7_3_2
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detail: 'Concatenating the \([[7,3,(d_X=3,d_Z=2)]]\) punctured hypercube code with the two-qubit phase-flip repetition code yields this \([[14,3,(d_X=3,d_Z=4)]]\) CSS phantom code \cite{arxiv:2601.20927}.'
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detail: 'Concatenating the \([[7,3,(d_X=3,d_Z=2)]]\) punctured hypercube code with the two-qubit phase-flip repetition code yields this \([[14,3,(d_X=3,d_Z=4)]]\) CSS phantom code \cite{arxiv:2601.20927}. Dual-rail concatenation of the same punctured hypercube code yields a single-qubit Clifford-equivalent CE CSS frame \cite{arxiv:2507.10395}.'
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- code_id: steane
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detail: 'Dual-rail concatenation of the \([[7,1,3]]\) Steane code yields a \([[14,1,3]]\) CE CSS code, from which the locally Clifford-equivalent \([[14,3,3]]\) CE CSS frame is obtained by removing two independent \(Z\)-type stabilizer generators \cite{arxiv:2507.10395}.'
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- code_id: quantum_repetition
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detail: 'The inner code in the construction is the two-qubit phase-flip repetition code \cite{arxiv:2601.20927}.'
Copy file name to clipboardExpand all lines: codes/quantum/qubits/stabilizer/qubit_stabilizer.yml
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detail: 'Stabilizer states on \(n\) qubits form complex projective 3-designs, but not 4-designs, on \(\mathbb{C}P^{2^n}\) \cite{arxiv:1510.02767}. The \hyperref[topic:clifford]{Clifford group} is a unitary 2-design \cite{arxiv:quant-ph/0103098} and a 3-design \cite[Thm. 1.6(B)]{arxiv:math/0502080}\cite[pg. 191]{doi:10.1007/3-540-30731-1}\cite{arxiv:1510.02619,arxiv:1510.02769} on \(U(2^n)\).'
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- code_id: iceberg
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detail: 'The \([[2m,2m-2,2]]\) code for \(2m\) being a multiple of four obstructs the Clifford group from being a 4-design \cite{arxiv:1609.08172}.'
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- code_id: constant_excitation
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detail: 'Concatenating the dual-rail code with an inner \([[n,k,d]]\) qubit stabilizer code yields a degenerate \([[2n,k,d]]\) constant-excitation stabilizer code that avoids coherent phase errors and is equivalent to a Pauli-rotated repetition-concatenated stabilizer code \cite{arxiv:2010.00538}.'
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- code_id: ampdamp
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detail: 'Concatenating the dual-rail code with an inner \([[n,k,d]]\) qubit stabilizer code yields a degenerate \([[2n,k,d]]\) constant-excitation stabilizer code that corrects \(d-1\) \hyperref[topic:ad]{AD} errors \cite{arxiv:1001.2356,arxiv:2010.00538}.'
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