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codes/classical/analog/sphere_packing/lattice/bw/leech.yml

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- code_id: golay
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detail: 'The Leech lattice can be obtained by lifting the Golay code to \(\mathbb{Z}_4\) \cite{doi:10.1109/18.312154}, appending a parity check, and applying \term{Construction \(A_4\)} \cite{doi:10.1007/3-540-57843-9_20} (see also \cite{doi:10.1098/rspa.1982.0071,doi:10.1007/978-1-4757-6568-7}). Half of the lattice can be obtained in a different construction \cite[Exam. 10.7.3]{preset:EricZin}.'
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- code_id: ternary_golay
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detail: 'The Leech lattice can be obtained by from the ternary Golay code \cite{doi:10.1098/rspa.1982.0071}.'
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detail: 'A 12-dimensional complex version of the Leech lattice can be obtained from the ternary Golay code \cite{doi:10.1016/0021-8693(83)90074-1,doi:10.1098/rspa.1982.0071}\cite[pg. 200]{doi:10.1007/978-1-4757-6568-7}.'
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- code_id: sharp_config
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detail: 'Several spherical sharp configrations are derived from the Leech lattice \cite{arxiv:math/0607446}.'
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- code_id: octacode

codes/quantum/oscillators/stabilizer/lattice/quantum_lattice.yml

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The \(m=2n\) case yields multimode GKP codes encoding a finite-dimensional logical subspace, while removing some displacements yields oscillator-into-oscillator GKP codes encoding an infinite-dimensional logical subspace. Codes defined on a hyper-rectangular lattice are \textit{CSS GKP} codes, and more general lattices, obtained by Gaussian transformations, yield non-CSS codes.
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notes:
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- 'Quantum lattice states are featured in the proof of hardness of LWE \cite[pg. 12]{doi:10.1145/1568318.1568324}.'
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- 'Quantum lattice states are featured in the proof of hardness of LWE \cite[pg. 12]{doi:10.1145/1568318.1568324} and the hidden subgroup problem over the reals \cite{doi:10.1145/2591796.2591860}.'
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- 'Single-mode quantum lattice states on a square lattice, otherwise known as square-lattice GKP states, are relevant to signal processing and condensed-matter physics; see the corresponding \hyperref[code:gkp]{code entry} for details.'
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codes/quantum/qubits/stabilizer/mbqc/cluster_state.yml

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detail: 'Kerdock codes correspond to cluster states, and the corresponding Clifford-group automorphisms of this set form a particular group \cite{doi:10.1112/S0024611597000403} that is a unitary 2-design on \(U(2^n)\) \cite{arxiv:1904.07842}. As such, cluster states form complex projective 2-designs on \(\mathbb{C}P^{2^n}\). These are useful in matrix-vector multiplication \cite{arxiv:2105.05879}.'
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- code_id: complex_projective
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detail: 'Kerdock codes correspond to cluster states, and the corresponding Clifford-group automorphisms of this set form a particular group \cite{doi:10.1112/S0024611597000403} that is a unitary 2-design on \(U(2^n)\) \cite{arxiv:1904.07842}. As such, cluster states form complex projective 2-designs on \(\mathbb{C}P^{2^n}\). These are useful in matrix-vector multiplication \cite{arxiv:2105.05879}.'
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- code_id: surface
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detail: 'Foliating the surface code yields a cluster state on the Lieb lattice \cite{arxiv:quant-ph/9707021,arxiv:1508.03468,arXiv:2211.01376,arXiv:2310.16032}.'
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# Kitaev writes about the larger lattice but doesn't call it Lieb lattice
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# In 1D, cluster states are examples of SPT phases with global symmetries and allow MBQC on a single qubit. In 2D, cluster states with subsystem symmetries are universal resources for MBQC. In 3D, cluster states with higher-form symmetries enable universal fault-tolerant MBQC.

codes/quantum/qudits/small/three_qutrit_permutation_invariant.yml

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code_id: three_qutrit_permutation_invariant
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name: '\(((3,3,2))_{3}\) Three-qutrit single-deletion code'
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name: '\(((3,2,2))_3\) Three-qutrit single-deletion code'
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introduced: '\cite{arxiv:2509.20545}'
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description: |
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Three-qutrit PI code that is the smallest qutrit PI code to correct one deletion error.
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The code admits the following logical codewords:
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\begin{align}
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|\overline{0}\rangle\propto&|000\rangle+|111\rangle+|222\rangle\\
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|\overline{1}\rangle\propto&|012\rangle+|021\rangle+|102\rangle+|120\rangle+|201\rangle+|210\rangle~.
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\end{align}
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The smallest qutrit PI code to correct one deletion error.
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