Recognition: 2 theorem links
· Lean TheoremGauss law codes and vacuum codes from lattice gauge theories
Pith reviewed 2026-05-10 19:23 UTC · model grok-4.3
The pith
Abelian lattice gauge theories produce quantum error correcting codes via quantum reference frames.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We develop a comprehensive framework for constructing quantum error correcting codes from Abelian lattice gauge theories using quantum reference frames as a unifying formalism. The codes fall into Gauss law codes that identify the code subspace with the full gauge-invariant sector and vacuum codes that restrict to the matter vacuum sector. For finite gauge groups vacuum codes are unitarily equivalent to pure gauge theory Gauss law codes, while for continuous groups this holds only after charge coarse-graining. Quantum reference frames characterize the algebraic structures and correctable error sets in all cases.
What carries the argument
Quantum reference frames as a unifying formalism to fully characterize the algebraic structures and correctable error sets of codes from Abelian lattice gauge theories.
If this is right
- In models with matter, the code space factors into gauge-invariant Wilson loops and dressed matter excitations.
- Errors in vacuum codes correspond to gauge-invariant charge excitations rather than Gauss law violations.
- The framework applies to arbitrary compact Abelian gauge groups and lattices in any dimension.
- When the gauge group is finite, vacuum codes are unitarily equivalent to pure gauge theory Gauss law codes.
Where Pith is reading between the lines
- This equivalence suggests that matter degrees of freedom can be integrated out to obtain equivalent error protection in pure gauge systems.
- The approach may allow quantum devices to simulate LGTs more robustly by using gauge invariance for error correction.
- Similar constructions might extend the parallelism between quantum error correction and gauge theory to non-Abelian cases.
Load-bearing premise
That quantum reference frames provide a complete and systematic characterization of the algebraic structures and correctable error sets for arbitrary compact Abelian gauge groups, lattices in any dimension, and both pure gauge and matter-coupled theories.
What would settle it
An explicit counterexample in which the quantum reference frame approach fails to identify the correct code subspace or correctable errors for some Abelian gauge group or lattice dimension.
Figures
read the original abstract
We develop a comprehensive framework for constructing quantum error correcting codes (QECCs) from Abelian lattice gauge theories (LGTs) using quantum reference frames (QRFs) as a unifying formalism. We consider LGTs with arbitrary compact Abelian gauge groups supported on lattices in arbitrary numbers of spatial dimensions, and we work with both pure gauge theories and theories with couplings to bosonic and fermionic matter. The codes that we construct fall into two classes: First, Gauss law codes identify the code subspace with the full gauge-invariant sector of the theory. In models with matter coupled to gauge fields, these codes inherit a natural subsystem structure in which gauge-invariant Wilson loops and dressed matter excitations factorize the code space. Second, vacuum codes restrict the code subspace to the matter vacuum sector within the gauge-invariant subspace, yielding codes where errors correspond to gauge-invariant charge excitations rather than to violations of the Gauss law. Despite their distinct setup, we show that when the gauge group is finite, vacuum codes are unitarily equivalent to pure gauge theory Gauss law codes, and that when the group is continuous, this is only true upon a charge coarse-graining of the vacuum code. In all cases, QRFs provide a systematic apparatus for fully characterizing the codes' algebraic structures and correctable error sets. For clarity, we illustrate our general results in $\mathbb{Z}_2$-gauge theory, as well as in scalar and fermionic QED. These findings offer fundamental insights into the parallelism between quantum error correction and gauge theory and point toward practical advantages for simulating LGTs on noisy quantum devices.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript develops a framework for constructing quantum error-correcting codes (QECCs) from Abelian lattice gauge theories (LGTs) on arbitrary-dimensional lattices with compact Abelian gauge groups, using quantum reference frames (QRFs) as the unifying formalism. It defines two classes of codes: Gauss law codes, which take the full gauge-invariant sector as the code subspace (with a natural subsystem structure when matter is coupled), and vacuum codes, which further restrict to the matter-vacuum sector so that errors correspond to gauge-invariant charge excitations. The paper claims that, for finite gauge groups, vacuum codes are unitarily equivalent to pure-gauge Gauss law codes; for continuous groups the equivalence holds only after charge coarse-graining. QRFs are used to characterize the algebraic structure and correctable error sets in all cases. Concrete illustrations are given for ℤ₂ gauge theory, scalar QED, and fermionic QED.
Significance. If the claimed equivalences and QRF-based characterizations hold, the work establishes a systematic bridge between gauge-invariant subspaces in LGTs and the code subspaces of QECCs, supplying both a general construction for arbitrary compact Abelian groups and explicit models. The unitary equivalence statements and the distinction between Gauss-law and vacuum codes provide concrete, falsifiable relations that could be tested in quantum simulations. The framework also suggests practical routes for encoding gauge-invariant information on noisy quantum hardware, which is a timely contribution given current efforts to simulate LGTs.
major comments (2)
- The abstract and introduction assert a general construction and an equivalence theorem for arbitrary compact Abelian groups and lattices in any dimension, yet the provided text supplies no explicit operator definitions, error-set proofs, or derivations of the unitary maps. A central load-bearing claim is therefore not yet verifiable from the manuscript as presented.
- § on vacuum-code equivalence (continuous-group case): the statement that equivalence holds only after 'charge coarse-graining' is introduced without a precise definition of the coarse-graining map or a demonstration that it preserves the correctable error set. This step is essential to the claimed distinction between finite and continuous cases.
minor comments (2)
- Notation for the QRF Hilbert-space decomposition and the gauge-invariant projector should be introduced once and used consistently; several passages reuse symbols without redefinition.
- The illustrations for scalar and fermionic QED are described at a high level; explicit Hamiltonians or stabilizer generators for the code subspaces would strengthen the concrete examples.
Simulated Author's Rebuttal
We thank the referee for their careful reading of our manuscript and for the constructive feedback. We address the major comments point by point below, indicating where revisions will be made to improve clarity and verifiability.
read point-by-point responses
-
Referee: The abstract and introduction assert a general construction and an equivalence theorem for arbitrary compact Abelian groups and lattices in any dimension, yet the provided text supplies no explicit operator definitions, error-set proofs, or derivations of the unitary maps. A central load-bearing claim is therefore not yet verifiable from the manuscript as presented.
Authors: We appreciate the referee's observation regarding the level of explicitness. The manuscript presents the general framework via the QRF formalism in Sections 3 and 4, along with statements of the equivalence theorems for finite and continuous groups. However, we agree that additional detail on operator definitions, derivations of the unitary maps, and proofs of the correctable error sets would strengthen verifiability. In the revised manuscript we will expand these sections to include explicit operator expressions for the code projectors and error operators, step-by-step derivations of the unitary equivalences for finite groups, and complete proofs that the error sets are preserved under the maps, covering arbitrary compact Abelian groups on lattices of any dimension. revision: yes
-
Referee: § on vacuum-code equivalence (continuous-group case): the statement that equivalence holds only after 'charge coarse-graining' is introduced without a precise definition of the coarse-graining map or a demonstration that it preserves the correctable error set. This step is essential to the claimed distinction between finite and continuous cases.
Authors: We concur that the charge coarse-graining step requires a more precise treatment. In the revised manuscript we will supply a formal definition of the coarse-graining map as the projection onto a discretized charge lattice (or an averaging operator over charge sectors) acting on the matter Hilbert space. We will then demonstrate explicitly that this map sends the correctable error set of the vacuum code to the correctable error set of the corresponding pure-gauge Gauss-law code, thereby establishing the claimed unitary equivalence for continuous groups. An illustrative calculation for the U(1) case in scalar QED will be added to make the construction concrete. revision: yes
Circularity Check
No significant circularity in the derivation chain
full rationale
The paper constructs Gauss law codes (identifying the code subspace with the full gauge-invariant sector) and vacuum codes (restricting to the matter vacuum sector) from Abelian LGTs via QRFs as a unifying formalism. The claimed unitary equivalences for finite groups and charge coarse-graining for continuous groups are derived algebraically within the framework, with explicit characterizations of algebraic structures and correctable error sets. Concrete illustrations in Z2-gauge theory, scalar QED, and fermionic QED are supplied directly. No load-bearing steps reduce by the paper's equations to self-definitions, fitted parameters renamed as predictions, or unverified self-citation chains; the QRF apparatus is applied as an external tool to organize standard gauge theory content rather than presupposing the target results.
Axiom & Free-Parameter Ledger
axioms (1)
- standard math Standard algebraic and representation-theoretic properties of compact Abelian gauge groups and quantum reference frames.
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquationwashburn_uniqueness_aczel unclearGauss law codes identify the code subspace with the full gauge-invariant sector... QRFs provide a systematic apparatus for fully characterizing the codes' algebraic structures and correctable error sets.
-
IndisputableMonolith/Foundation/DimensionForcingalexander_duality_circle_linking unclearWe show that when the gauge group is finite, vacuum codes are unitarily equivalent to pure gauge theory Gauss law codes
Reference graph
Works this paper leans on
-
[1]
Charge superselection rule,
Y. Aharonov and L. Susskind, “Charge superselection rule,”Phys. Rev.155(1967) 1428–1431
1967
-
[2]
Quantum frames of reference,
Y. Aharonov and T. Kaufherr, “Quantum frames of reference,”Phys. Rev. D30(1984) 368–385. 91
1984
-
[3]
Evolution without evolution: Dynamics described by stationary observables,
D. N. Page and W. K. Wootters, “Evolution without evolution: Dynamics described by stationary observables,”Phys. Rev. D27(1983) 2885–2892
1983
-
[4]
Quantum theory of gravity. I. The canonical theory,
B. S. DeWitt, “Quantum theory of gravity. I. The canonical theory,”Phys. Rev.160(1967) 1113–1148
1967
-
[5]
Quantum reference systems,
C. Rovelli, “Quantum reference systems,”Class. Quant. Grav.8(1991) 317–332
1991
-
[6]
Partial observables,
C. Rovelli, “Partial observables,”Phys. Rev. D65(2002) 124013
2002
-
[7]
Reference frames, superselection rules, and quantum information
S. D. Bartlett, T. Rudolph, and R. W. Spekkens, “Reference frames, superselection rules, and quantum information,”Rev. Mod. Phys.79(2007) 555–609,arXiv:quant-ph/0610030
work page Pith review arXiv 2007
-
[8]
Quantum mechanics and the covariance of physical laws in quantum reference frames,
F. Giacomini, E. Castro-Ruiz, and v. Brukner, “Quantum mechanics and the covariance of physical laws in quantum reference frames,”Nat. Commun.10no. 1, (2019)
2019
-
[9]
A.-C. de la Hamette, T. D. Galley, P. A. H¨ ohn, L. Loveridge, and M. P. M¨ uller, “Perspective-neutral approach to quantum frame covariance for general symmetry groups,” arXiv:2110.13824 [quant-ph]
-
[10]
Quantum Frame Relativity of Subsystems, Correlations and Thermodynamics,
P. A. H¨ ohn, I. Kotecha, and F. M. Mele, “Quantum Frame Relativity of Subsystems, Correlations and Thermodynamics,”arXiv:2308.09131 [quant-ph]
-
[11]
A. Vanrietvelde, P. A. H¨ ohn, F. Giacomini, and E. Castro-Ruiz, “A change of perspective: switching quantum reference frames via a perspective-neutral framework,”Quantum4(2020) 225,arXiv:1809.00556 [quant-ph]
-
[12]
S. Ali Ahmad, T. D. Galley, P. A. H¨ ohn, M. P. E. Lock, and A. R. H. Smith, “Quantum Relativity of Subsystems,”Phys. Rev. Lett.128no. 17, (2022) 170401,arXiv:2103.01232 [quant-ph]
-
[13]
G. Ara´ ujo-Regado, P. A. H¨ ohn, and F. Sartini, “Relational entanglement entropies and quantum reference frames in gauge theories,”arXiv:2506.23459 [hep-th]
-
[14]
Operational Quantum Reference Frame Transformations,
T. Carette, J. G lowacki, and L. Loveridge, “Operational Quantum Reference Frame Transformations,”Quantum9(2025) 1680,arXiv:2303.14002 [quant-ph]
-
[15]
Interpreting quantum reference frame transformations through a simple example,
E. Castro-Ruiz, T. D. Galley, and L. Loveridge, “Interpreting quantum reference frame transformations through a simple example,”arXiv:2508.09540 [quant-ph]
-
[16]
S. Carrozza and P. A. H¨ ohn, “Edge modes as reference frames and boundary actions from post-selection,”JHEP02(2022) 172,arXiv:2109.06184 [hep-th]
-
[17]
Soft edges: the many links between soft and edge modes,
G. Ara´ ujo-Regado, P. A. H¨ ohn, F. Sartini, and B. Tomova, “Soft edges: the many links between soft and edge modes,”JHEP07(2025) 180,arXiv:2412.14548 [hep-th]
-
[18]
Local subsystems in gauge theory and gravity,
W. Donnelly and L. Freidel, “Local subsystems in gauge theory and gravity,”JHEP2016no. 9, (2016)
2016
-
[19]
C. J. Fewster, D. W. Janssen, and K. Rejzner, “Semi-local observables, edge modes and quantum reference frames in quantum electromagnetism: an algebraic approach,”arXiv:2508.20939 [math-ph]
-
[20]
Fighting non-locality with non-locality: microcausality and boundary conditions in QED,
P. A. H¨ ohn and J. Kirklin, “Fighting non-locality with non-locality: microcausality and boundary conditions in QED,”arXiv:2512.16898 [hep-th]. 92
-
[21]
C. Goeller, P. A. H¨ ohn, and J. Kirklin, “Diffeomorphism-invariant observables and dynamical frames in gravity: reconciling bulk locality with general covariance,”arXiv:2206.01193 [hep-th]
-
[22]
J. De Vuyst, S. Eccles, P. A. H¨ ohn, and J. Kirklin, “Gravitational entropy is observer-dependent,”JHEP07(2025) 146,arXiv:2405.00114 [hep-th]
-
[23]
Gravitational null rays: Covariant Quantization and the Dressing Time
L. Freidel and J. Kirklin, “Gravitational null rays: Covariant Quantization and the Dressing Time,”arXiv:2604.02228 [hep-th]
work page internal anchor Pith review Pith/arXiv arXiv
-
[24]
Quantum coordinates, localisation of events, and the quantum hole argument,
V. Kabel, A.-C. de la Hamette, L. Apadula, C. Cepollaro, H. Gomes, J. Butterfield, and ˇC. Brukner, “Quantum coordinates, localisation of events, and the quantum hole argument,” Commun. Phys.8no. 1, (2025) 185,arXiv:2402.10267 [quant-ph]
-
[25]
A correspondence between quantum error correcting codes and quantum reference frames,
S. Carrozza, A. Chatwin-Davies, P. A. H¨ ohn, and F. M. Mele, “A correspondence between quantum error correcting codes and quantum reference frames,”arXiv:2412.15317 [quant-ph]
-
[26]
Fault-tolerant quantum computation by anyons
A. Y. Kitaev, “Fault tolerant quantum computation by anyons,”Annals Phys.303(2003) 2–30, arXiv:quant-ph/9707021
work page Pith review arXiv 2003
-
[27]
Quantum codes on a lattice with boundary
S. B. Bravyi and A. Y. Kitaev, “Quantum codes on a lattice with boundary,” arXiv:quant-ph/9811052
-
[28]
Confinement of Quarks,
K. G. Wilson, “Confinement of Quarks,”Phys. Rev. D10(1974) 2445–2459
1974
-
[29]
Hamiltonian Formulation of Wilson’s Lattice Gauge Theories,
J. B. Kogut and L. Susskind, “Hamiltonian Formulation of Wilson’s Lattice Gauge Theories,” Phys. Rev. D11(1975) 395–408
1975
-
[30]
An Introduction to Lattice Gauge Theory and Spin Systems,
J. B. Kogut, “An Introduction to Lattice Gauge Theory and Spin Systems,”Rev. Mod. Phys.51 (1979) 659
1979
-
[31]
Gauss’ law code,
“Gauss’ law code,” inThe Error Correction Zoo, V. V. Albert and P. Faist, eds. 2024. https://errorcorrectionzoo.org/c/gauss_law
2024
- [32]
-
[33]
Fault-tolerant simulation of Lattice Gauge Theories with gauge covariant codes,
L. Spagnoli, A. Roggero, and N. Wiebe, “Fault-tolerant simulation of Lattice Gauge Theories with gauge covariant codes,”Quantum10(2026) 1968,arXiv:2405.19293 [quant-ph]
-
[34]
Qudit stabiliser codes forZ N lattice gauge theories with matter,
L. Spagnoli, A. Roggero, and N. Wiebe, “Qudit stabiliser codes forZ N lattice gauge theories with matter,”arXiv:2602.20661 [quant-ph]
-
[35]
Quantum Error Correction Codes for Truncated SU(2) Lattice Gauge Theories,
X. Yao, “Quantum Error Correction Codes for Truncated SU(2) Lattice Gauge Theories,” arXiv:2511.13721 [quant-ph]
-
[36]
Simulating physics with computers,
R. P. Feynman, “Simulating physics with computers,”Int. J. Theor. Phys.21no. 6, (1982) 467–488
1982
-
[37]
Universal quantum simulators,
S. Lloyd, “Universal quantum simulators,”Science273(1996) 1073–1078
1996
-
[38]
I. M. Georgescu, S. Ashhab, and F. Nori, “Quantum simulation,”Rev. Mod. Phys.86no. 1, (2014) 153–185.http://dx.doi.org/10.1103/RevModPhys.86.153. 93
-
[39]
Quantum Simulators: Architectures and Opportunities,
E. Altman et al., “Quantum Simulators: Architectures and Opportunities,”PRX Quantum2 no. 1, (2021) 017003,arXiv:1912.06938 [quant-ph]
-
[40]
Practical quantum advantage in quantum simulation,
A. J. Daley, I. Bloch, C. Kokail, S. Flannigan, N. Pearson, M. Troyer, and P. Zoller, “Practical quantum advantage in quantum simulation,”Nature607no. 7920, (2022) 667–676
2022
-
[41]
Lattice QCD and heavy ion collisions: a review of recent progress,
C. Ratti, “Lattice QCD and heavy ion collisions: a review of recent progress,”Rept. Prog. Phys. 81no. 8, (2018) 084301,arXiv:1804.07810 [hep-lat]
-
[42]
Review of Baryon Spectroscopy in Lattice QCD,
H.-W. Lin, “Review of Baryon Spectroscopy in Lattice QCD,”Chin. J. Phys.49(2011) 827, arXiv:1106.1608 [hep-lat]
-
[43]
Philipsen, The QCD equation of state from the lattice, Prog
O. Philipsen, “The QCD equation of state from the lattice,”Prog. Part. Nucl. Phys.70(2013) 55–107,arXiv:1207.5999 [hep-lat]
-
[44]
Thermodynamics of strong-interaction matter from Lattice QCD,
H.-T. Ding, F. Karsch, and S. Mukherjee, “Thermodynamics of strong-interaction matter from Lattice QCD,”Int. J. Mod. Phys. E24no. 10, (2015) 1530007,arXiv:1504.05274 [hep-lat]
-
[45]
Aarts, Introductory lectures on lattice QCD at nonzero baryon number, J
G. Aarts, “Introductory lectures on lattice QCD at nonzero baryon number,”J. Phys. Conf. Ser. 706no. 2, (2016) 022004,arXiv:1512.05145 [hep-lat]
-
[46]
Nagata, Finite-density lattice QCD and sign prob- lem: current status and open problems, Prog
K. Nagata, “Finite-density lattice QCD and sign problem: Current status and open problems,” Prog. Part. Nucl. Phys.127(2022) 103991,arXiv:2108.12423 [hep-lat]
-
[47]
Bañuls et al.,Simulating Lattice Gauge Theories within Quantum Technologies,Eur
M. C. Ba˜ nuls et al., “Simulating Lattice Gauge Theories within Quantum Technologies,”Eur. Phys. J. D74no. 8, (2020) 165,arXiv:1911.00003 [quant-ph]
- [48]
- [49]
-
[50]
A. Di Meglio et al., “Quantum Computing for High-Energy Physics: State of the Art and Challenges,”PRX Quantum5no. 3, (2024) 037001,arXiv:2307.03236 [quant-ph]
-
[51]
Quantum error thresholds for gauge-redundant digitizations of lattice field theories,
M. Carena, H. Lamm, Y.-Y. Li, and W. Liu, “Quantum error thresholds for gauge-redundant digitizations of lattice field theories,”Phys. Rev. D110no. 5, (2024) 054516,arXiv:2402.16780 [hep-lat]
-
[52]
Oracles for Gauss’s law on digital quantum computers,
J. R. Stryker, “Oracles for Gauss’s law on digital quantum computers,”Phys. Rev. A99no. 4, (2019) 042301,arXiv:1812.01617 [quant-ph]
-
[53]
Solving Gauss’s Law on Digital Quantum Computers with Loop-String-Hadron Digitization,
I. Raychowdhury and J. R. Stryker, “Solving Gauss’s Law on Digital Quantum Computers with Loop-String-Hadron Digitization,”Phys. Rev. Res.2no. 3, (2020) 033039,arXiv:1812.07554 [hep-lat]
-
[54]
Trade-offs in Gauss’s law error correction for lattice gauge theory quantum simulations,
B. Pato and N. Klco, “Trade-offs in Gauss’s law error correction for lattice gauge theory quantum simulations,”arXiv:2602.22121 [quant-ph]
-
[55]
A Theory of quantum error correcting codes,
E. Knill and R. Laflamme, “A Theory of quantum error correcting codes,”Phys. Rev. Lett.84 (2000) 2525–2528,arXiv:quant-ph/9604034
-
[56]
Fault-tolerant quantum computation against biased noise,
P. Aliferis and J. Preskill, “Fault-tolerant quantum computation against biased noise,”Phys. Rev. A78no. 5, (2008) . 94
2008
-
[57]
Bias-preserving gates with stabilized cat qubits,
S. Puri et al., “Bias-preserving gates with stabilized cat qubits,”Sci. Adv.6no. 34, (2020) aay5901,arXiv:1905.00450 [quant-ph]
-
[58]
E. Rothlin,Exploring the Connection between Gauge Theory and Quantum Error Correction via Quantum Reference Frames. PhD thesis, ETH Zurich, 2025. https://doi.org/10.3929/ethz-c-000784853
-
[59]
Error correction in lattice quantum electrodynamics with quantum reference frames,
E. Rothlin, C. Ferradini, and L.-Q. Chen, “Error correction in lattice quantum electrodynamics with quantum reference frames,”simultaneously submitted to the arXiv(2026)
2026
-
[60]
Stabilizer Codes and Quantum Error Correction
D. Gottesman, “Stabilizer codes and quantum error correction,”arXiv:quant-ph/9705052
work page internal anchor Pith review arXiv
-
[61]
M. A. Nielsen and I. L. Chuang,Quantum Computation and Quantum Information. Cambridge University Press, 10th ed., 2010
2010
-
[62]
D. Gottesman, “An Introduction to Quantum Error Correction and Fault-Tolerant Quantum Computation,”arXiv:0904.2557 [quant-ph]
-
[63]
Quantum error correction on infinite-dimensional hilbert spaces,
C. B´ eny, A. Kempf, and D. W. Kribs, “Quantum error correction on infinite-dimensional hilbert spaces,”J. Math. Phys.50no. 6, (2009)
2009
-
[64]
Entropy gain and the choi-jamiolkowski correspondence for infinite-dimensional quantum evolutions,
A. S. Holevo, “Entropy gain and the choi-jamiolkowski correspondence for infinite-dimensional quantum evolutions,”Theor. Math. Phys.166no. 1, (2011) 123–138
2011
-
[65]
Standard form of qudit stabilizer groups,
V. Gheorghiu, “Standard form of qudit stabilizer groups,”Phys. Lett. A378no. 5-6, (2014) 505–509,arXiv:1101.1519 [quant-ph]
-
[66]
E. M. Rains, “Nonbinary quantum codes,”IEEE Trans. Info. Theor.45no. 6, (1999) 1827–1832, arXiv:quant-ph/9703048
-
[67]
302–313, arXiv:quant-ph/9802007 [quant-ph]
D. Gottesman, “Fault tolerant quantum computation with higher dimensional systems,”Chaos Solitons Fractals10(1999) 1749–1758,arXiv:quant-ph/9802007
-
[68]
Nonbinary quantum stabilizer codes,
A. Ashikhmin and E. Knill, “Nonbinary quantum stabilizer codes,”IEEE Trans. Info. Theor.47 no. 7, (2001) 3065–3072,arXiv:quant-ph/0005008
-
[69]
Modular-qudit stabilizer code,
“Modular-qudit stabilizer code,” inThe Error Correction Zoo, V. V. Albert and P. Faist, eds. 2022.https://errorcorrectionzoo.org/c/qudit_stabilizer
2022
-
[70]
Qudits and High-Dimensional Quantum Computing,
Y. Wang, Z. Hu, B. C. Sanders, and S. Kais, “Qudits and High-Dimensional Quantum Computing,”Front. in Phys.8(2020) 589504,arXiv:2008.00959 [quant-ph]
-
[71]
Operator quantum error-correcting subsystems for self-correcting quantum memories,
D. Bacon, “Operator quantum error-correcting subsystems for self-correcting quantum memories,”Phys. Rev. A73no. 1, (2006) 012340,arXiv:quant-ph/0506023
-
[72]
Scheme for reducing decoherence in quantum computer memory,
P. W. Shor, “Scheme for reducing decoherence in quantum computer memory,”Phys. Rev. A52 no. 4, (1995) R2493–R2496
1995
-
[73]
Operator quantum error correction,
D. W. Kribs, R. Laflamme, D. Poulin, and M. Lesosky, “Operator quantum error correction,” Quant. Inf. Comput.6no. 4-5, (2006) 382–399,arXiv:quant-ph/0504189
-
[74]
Stabilizer formalism for operator quantum error correction,
D. Poulin, “Stabilizer formalism for operator quantum error correction,”Phys. Rev. Lett.95 no. 23, (2005) . 95
2005
-
[75]
Simulating lattice gauge theories on a quantum computer
T. Byrnes and Y. Yamamoto, “Simulating lattice gauge theories on a quantum computer,”Phys. Rev. A73(2006) 022328,arXiv:quant-ph/0510027
work page Pith review arXiv 2006
- [76]
-
[77]
E. Zohar, “Quantum simulation of lattice gauge theories in more than one space dimension—requirements, challenges and methods,”Phil. Trans. A. Math. Phys. Eng. Sci.380 no. 2216, (2021) 20210069,arXiv:2106.04609 [quant-ph]
-
[78]
F. Giacomini, E. Castro-Ruiz, and ˇC. Brukner, “Quantum mechanics and the covariance of physical laws in quantum reference frames,”Nature Commun.10no. 1, (2019) 494, arXiv:1712.07207 [quant-ph]
-
[79]
Gauss’ law code
“Gauss’ law code.”https://errorcorrectionzoo.org/c/gauss_law. The Error Correction Zoo
-
[80]
The Reconstruction of Gauge Potentials From Wilson Loops,
R. Giles, “The Reconstruction of Gauge Potentials From Wilson Loops,”Phys. Rev. D24(1981) 2160
1981
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.