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codes/quantum/qudits_galois/stabilizer/evaluation/quantum_ag.yml
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####################################################### | ||
## This is a code entry in the error correction zoo. ## | ||
## https://github.com/errorcorrectionzoo ## | ||
####################################################### | ||
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code_id: quantum_ag | ||
physical: galois | ||
logical: galois | ||
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name: 'Quantum AG code' | ||
introduced: '\cite{arxiv:quant-ph/0107129}' | ||
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description: | | ||
A Galois-qudit CSS code constructed using two linear AG codes. | ||
features: | ||
rate: 'Quantum AG codes \cite{arxiv:quant-ph/0107129} can be asymptotically good. There exist three such families \cite{arxiv:2408.07764,arxiv:2408.09254,arxiv:2408.10140} that admit a diagonal transversal gate at the third level of the \term{Clifford hierarchy}.' | ||
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magic_scaling_exponent: 'By defining a generalization of triorthogonal matrices to Galois qudits of dimension \(q=2^m\), one can construct an asymptotically good family of quantum AG codes that admits a diagonal transversal gate at the third level of the \term{Clifford hierarchy} and attains a zero magic-state yield parameter, \(\gamma = 0\) \cite{arxiv:2408.07764}. This code can be treated as a qubit code by decomposing each Galois qudit into a Kronecker product of \(m\) qubits; see \cite{doi:10.1109/18.959288}\cite[Sec. 5.3]{arxiv:quant-ph/0501074}\cite{preset:GottesmanBook}. Two other such asymptotically good families exist \cite{arxiv:2408.09254,arxiv:2408.10140}, admitting a different diagonal gate at the third level of the \term{Clifford hierarchy}.' | ||
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encoders: | ||
- 'Encoding defined in Ref. \cite{arxiv:quant-ph/0107129} uses a technique from Ref. \cite{arxiv:quant-ph/0005008} to encode quantum stabilizer codes.' | ||
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transversal_gates: | ||
- 'There exist three asymptotically good code families \cite{arxiv:2408.07764,arxiv:2408.09254,arxiv:2408.10140} that admit a diagonal transversal gate at the third level of the \term{Clifford hierarchy}.' | ||
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relations: | ||
parents: | ||
- code_id: galois_css | ||
detail: 'Quantum AG codes can be realized in the CSS code construction \cite{doi:10.1007/s11128-006-0047-9}.' | ||
cousins: | ||
- code_id: ag | ||
- code_id: quantum_triorthogonal | ||
detail: 'By defining a generalization of triorthogonal matrices to Galois qudits of dimension \(q=2^m\), one can construct an asymptotically good family of quantum AG codes that admits a diagonal transversal gate at the third level of the \term{Clifford hierarchy} and attains a zero magic-state yield parameter, \(\gamma = 0\) \cite{arxiv:2408.07764}. This code can be treated as a qubit code by decomposing each Galois qudit into a Kronecker product of \(m\) qubits; see \cite{doi:10.1109/18.959288}\cite[Sec. 5.3]{arxiv:quant-ph/0501074}\cite{preset:GottesmanBook}. Two other such asymptotically good families exist \cite{arxiv:2408.09254,arxiv:2408.10140}, admitting a different diagonal gate at the third level of the \term{Clifford hierarchy}.' | ||
- code_id: shimura | ||
detail: 'The AG codes used in an asymptotically good construction of quantum AG codes with non-Clifford transversal gates \cite{arxiv:2408.09254} are those of the TVZ codes.' | ||
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# Begin Entry Meta Information | ||
_meta: | ||
# Change log - most recent first | ||
changelog: | ||
- user_id: VictorVAlbert | ||
date: '2024-08-23' |
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